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WO2025042329A1 - Déphaseur et son procédé de formation - Google Patents

Déphaseur et son procédé de formation Download PDF

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Publication number
WO2025042329A1
WO2025042329A1 PCT/SG2023/050578 SG2023050578W WO2025042329A1 WO 2025042329 A1 WO2025042329 A1 WO 2025042329A1 SG 2023050578 W SG2023050578 W SG 2023050578W WO 2025042329 A1 WO2025042329 A1 WO 2025042329A1
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WO
WIPO (PCT)
Prior art keywords
region
slab waveguide
waveguide
silicon
phase shifter
Prior art date
Application number
PCT/SG2023/050578
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English (en)
Inventor
Leh Woon LIM
Yao Ting Lennon LEE
Original Assignee
Agency For Science, Technology And Research
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Priority to PCT/SG2023/050578 priority Critical patent/WO2025042329A1/fr
Publication of WO2025042329A1 publication Critical patent/WO2025042329A1/fr

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    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/015—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on semiconductor elements having potential barriers, e.g. having a PN or PIN junction
    • G02F1/025—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on semiconductor elements having potential barriers, e.g. having a PN or PIN junction in an optical waveguide structure
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122—Basic optical elements, e.g. light-guiding paths
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/13—Integrated optical circuits characterised by the manufacturing method
    • G02B6/136—Integrated optical circuits characterised by the manufacturing method by etching
    • G—PHYSICS
    • G02—OPTICS
    • G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/21—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  by interference
    • G02F1/225—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  by interference in an optical waveguide structure

Definitions

  • Various embodiments of this disclosure may relate to a phase shifter.
  • Various embodiments of this disclosure may relate to a method of forming a phase shifter.
  • Signal transmission is often accomplished by modulation of an optical carrier signal using electro-optical modulators. This is commonly done using a method of intensity modulation with a Mach Zehnder-based interferometric modulator, which includes an input waveguide, an optical splitter, two optical signal paths where one or both contain a phaseshifting element (i.e. phase shifter), an optical combiner, and an output waveguide.
  • a Mach Zehnder-based interferometric modulator which includes an input waveguide, an optical splitter, two optical signal paths where one or both contain a phaseshifting element (i.e. phase shifter), an optical combiner, and an output waveguide.
  • phaseshifting element i.e. phase shifter
  • the intensity of the optical signal at the Mach-Zehnder modulator output is a result of interference effects where the phase of the optical carrier in one path is changed with respect to the other optical path.
  • An alternative method of signal transmission is to employ an analog optical link.
  • a radio frequency signal provided by a radio frequency source, is imposed onto the optical carrier signal, provided by an optical source such as a laser and using an electro-optic modulator such as Mach-Zehnder modulator.
  • the modulated optical signal is then transmitted from one location to another by fiber optics network.
  • This method of signal transmission is advantageous compared to currently employed methods to reduce the number of components in the optical link, which translates to reduction in complexity, cost, power consumption.
  • analog optical links are limited by non-linear impairments due to the non-linear output response of the modulator and transmission properties in optical fibers.
  • the linearity of the modulator would be required to be sufficiently high to prevent significant distortions, the third order intermodulation distortions occurring at frequencies overlapping with the transmitted radio frequencies (RF) of interest.
  • the Mach-Zehnder modulator transfer function is inherently non-linear.
  • proposed approaches to suppress the third order intermodulation signals i.e., to increase the spurious free dynamic range of the Mach-Zehnder modulator, involve introduction of another source of non-linearity by means of electronic or optical techniques such as applying predistortion, employing series/parallel multiple Mach-Zehnder modulator configuration or inherent material non-linear electro-optical effects.
  • third order intermodulation suppression can be achieved through two Mach-Zehnder modulators connected in parallel.
  • the frequency responses of both Mach-Zehnder modulators are required to be as similar as possible and the input electrical signals to both Mach-Zehnder modulators require precise amplitude and phase relationship, both of which are challenging to realize at scale which will be required for future communication networks.
  • QCSE Quantum-Confined Stark Effect
  • electro-absorption modulators work by intensity modulation, i.e., 0V gives a T' state and ⁇ 0V gives a 'O' state.
  • QCSE devices contain quantum well layers that are each sandwiched by quantum barrier layers whereby the well material has a bandgap narrower than the barrier material.
  • germanium Ge
  • silicon-germanium Sii- x Ge x or simply SiGe
  • the SiGe barrier layer is required to have high concentration of Ge.
  • the QCSE effect relies on the band tilting phenomenon due to applied electric field in the perpendicular direction of pn junction to produce the red shift in absorption spectrum under applied bias.
  • the phase shifter may include rib waveguide.
  • the rib waveguide may include a base.
  • the rib waveguide may further include a stacked arrangement on the base, the stacked arrangement including alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the phase shifter may also include a first slab waveguide region and a second slab waveguide region.
  • a first region of the rib waveguide, the first region of the rib waveguide including a first region of the base and a first region of the stacked arrangement, may be a doped region having a first type conductivity.
  • a second region of the rib waveguide adjoining the first region of the rib waveguide, the second region of the rib waveguide including a second region of the base and a second region of the stacked arrangement may be a doped region having a second type conductivity opposite to the first type conductivity.
  • the first slab waveguide region, the first slab waveguide region adjoining the first region of the base may be a doped region having the first type conductivity.
  • the second slab waveguide region, the second slab waveguide region adjoining the second region of the base may be a doped region having the second type conductivity.
  • Various embodiments may include a method of forming a phase shifter.
  • the method may include forming a rib waveguide.
  • the rib waveguide may include a base, and a stacked arrangement on the base, the stacked arrangement including alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the method may also include forming a first slab waveguide region.
  • the method may further include forming a second slab waveguide region.
  • a first region of the rib waveguide, the first region of the rib waveguide including a first region of the base and a first region of the stacked arrangement may be a doped region having a first type conductivity.
  • a second region of the rib waveguide adjoining the first region of the rib waveguide, the second region of the rib waveguide including a second region of the base and a second region of the stacked arrangement is a doped region having a second type conductivity opposite to the first type conductivity.
  • the first slab waveguide region, the first slab waveguide region adjoining the first region of the base may be a doped region having the first type conductivity.
  • the second slab waveguide region, the second slab waveguide region adjoining the second region of the base may be a doped region having the second type conductivity.
  • FIG. 1A shows the existing 5G fronthaul network architecture.
  • FIG. IB shows the proposed 6G fronthaul network architecture enabled by a high linearity photonic modulator according to various embodiments.
  • FIG. 1C shows a schematic illustrating the modulator being a non-linear device.
  • FIG. ID shows a plot of output power (in decibels -milliwatts or dBm) as a function of input power (in decibels-milliwatts or dBm) illustrating derivation of the spurious free dynamic range (SFDR) according to various embodiments.
  • FIG. 2 shows a general illustration of a phase shifter according to various embodiments.
  • FIG. 3 A shows a general illustration of a method of forming a phase shifter according to various embodiments.
  • FIG. 3B shows another illustration of a method of forming a phase shifter according to various embodiments.
  • FIG. 4A shows a cross-sectional schematic of a phase shifter according to various embodiments.
  • FIG. 4B shows a modulator in which the phase shifter is arranged along one of the two optical arms of the modulator according to various embodiments.
  • FIG. 5A shows a top silicon (Si) layer of a silicon-on-insulator (SOI) substrate according to various embodiments.
  • FIG. 5B shows the silicon (Si) layer after etching according to various embodiments.
  • FIG. 5C shows the patterning of the silicon oxide layer to form the trench according to various embodiments.
  • FIG. 5D shows the formation of the stacked arrangement of the rib waveguide according to various embodiments.
  • FIG. 5E shows the formation of doped regions in the rib waveguide and doped slab waveguide regions according to various embodiments.
  • FIG. 5F shows forming of the cladding according to various embodiments.
  • FIG. 5G shows the forming of the electrodes according to various embodiments.
  • FIG. 6A shows the formation of stack according to various embodiments.
  • FIG. 6B shows the formation of the photoresist structure according to various embodiments.
  • FIG. 6C shows the formation of the stacked arrangement according to various embodiments.
  • FIG. 6D shows the formation of doped regions in the rib waveguide and doped slab waveguide regions according to various embodiments.
  • FIG. 6E shows forming of the cladding according to various embodiments.
  • FIG. 6F shows the forming of the electrodes according to various embodiments.
  • FIG. 7 shows (top) a plot of thickness (in nanometers or nm) as a function of number of periods illustrating the variation of spurious free dynamic range (SFDR) (decibels relative to carrier Hertz to power of two-thirds or dBc. Hz 2/3 ) for Sio.gGeo.i according to various embodiments; (middle) a plot of thickness (in nanometers or nm) as a function of number of periods illustrating the variation of spurious free dynamic range (SFDR) (decibels relative to carrier Hertz to power of two-thirds or dBc.
  • SFDR spurious free dynamic range
  • the articles “a”, “an” and “the” as used with regard to a feature or element include a reference to one or more of the features or elements.
  • the term “about” or “approximately” as applied to a numeric value encompasses the exact value and a reasonable variance, e.g. within 10% of the specified value.
  • Embodiments described in the context of one of the phase shifters or modulators are analogously valid for the other phase shifters or modulators, embodiments described in the context of a method are analogously valid for a phase shifter/modulator, and vice versa.
  • ARoF digital radio over fiber fronthaul
  • 5G severely lags behind due to limitations originating from the fronthaul network architecture used in existing wireless communications network links, i.e. digital radio over fiber (DRoF).
  • DRIF digital radio over fiber
  • An analog radio over fiber fronthaul (ARoF) may be needed to achieve significant improvements to data capacity and latencies.
  • Advantages of ARoF may include greater data capacity (50x) and lower latency (50x) at reduced costs (7x), power consumption (3x) and footprint (2x).
  • the key enabling component for ARoF may be a high linearity photonic modulator, e.g. with spurious free dynamic range (SFDR) > 130 dBc. Hz 2/3 .
  • FIG. 1A shows the existing 5G fronthaul network architecture.
  • FIG. IB shows the proposed 6G fronthaul network architecture enabled by a high linearity photonic modulator according to various embodiments.
  • FIG. 1C shows a schematic illustrating the modulator being a non-linear device.
  • one or more non-linear compensation techniques are used: (1) operating two modulators in series or parallel; (2) injecting electronic pre-distortion signals; and/or (3) using a material’s inherent electro-optic effects.
  • the disadvantages may come from either requiring identical frequency responses from two devices, complicated device fabrication methods to incorporate III-V/LiNbOs on silicon or specific electrical operating conditions governed by complex circuit design.
  • the system linearity may be limited by the SFDR which primarily comes from non-linearities generated by the electro-optics (EO) modulator.
  • the SFDR may be defined as the range between the smallest signal that can be detected (just above noise floor) and the largest distortion-free signal.
  • FIG. ID shows a plot of output power (in decibels-milliwatts or dBm) as a function of input power (in decibels-milliwatts or dBm) illustrating derivation of the spurious free dynamic range
  • SFDR ⁇ (OIP 3 — A/ o ) as shown in
  • FIG. ID. may relate to a multi-layered silicon-germanium/silicon (SixGei-x/Si) modulator that can achieve a high SFDR, e.g. SFDR > 130 dBc. Hz 2/3 .
  • the high SFDR photonic modulator may be the key enabling component for an ARoF link.
  • phase shifter (alternatively referred to as a phase shifting device or a phase shifter device) for use in one or both optical paths of the Mach-
  • Silicon germanium layers may be introduced into the rib waveguides in the Mach Zehnder modulators.
  • Third order intermodulation distortions may be suppressed by non-linear free carrier plasma dispersion effect present in the structure.
  • the structure may demonstrate the ability to achieve spurious free dynamic range of above 130 dBc. Hz 2/3 . This may be obtained through tuning of the germanium (Ge) composition, thickness and strain in the waveguide section which alters the free carrier properties including effective conductivity mass, mobility, and dielectric constant.
  • Modulation is achieved in Mach Zehnder modulators when the phase change of the propagating optical wave in one optical path results in a net intensity change due to interference effects with the other optical path at the modulator output.
  • the phase changing element may typically be a pn junction, which forms a depletion region of immobile ions and free carriers in the vicinity, in a rib waveguide geometry that confines the optical wave. Hence, the optical wave interacts with free carriers along the length of the phase shifter.
  • the refractive index (and hence the phase of the optical wave) is tuned by changing the number of free carriers interacting with the optical wave which can be achieved through applying a voltage bias to the phase shifter.
  • the change in refractive index, An is related to the number free carriers and their conductivity effect masses as expressed by the Drude model: where e is the elementary charge, A is the wavelength of light, c is the speed of light in vacuum, so is the vacuum permittivity, n is the refractive index, AN e is the change in free electron concentration, AN ft is the change in free hole concentration, m c * e is the conductivity effective mass of electrons and m c * h is the conductivity effective mass of holes.
  • the change in refractive index may be inversely proportional to the conductivity effective masses.
  • the conductivity effective masses can be tuned by strain engineering. For example, growth of SiGe on Si produces a strained SiGe film due to the lattice constant mismatch between SiGe and Si, since the lattice constant of Ge is larger than Si by 4%. Strain effects alter the conductivity effective masses in SiGe because of valence band splitting, where the heavy hole band shifts to an energy level above light hole band, giving rise to a reduced conductivity effective mass. The thickness of SiGe film on Si should be kept below the critical thickness limit to maintain the strain profile.
  • Various embodiments may relate to a phase shifter including a stacked arrangement of alternating layers of SiGe and Si, which produces a specific refractive index change profile in the waveguide region to enhance the free carrier effects by tuning the Ge composition and layer thicknesses while maintaining strain in each layer.
  • the phase shifter is based on reverse biased depletion structure.
  • the pn junction may be created at the center of the waveguide with the electrodes (on two far ends of the slab waveguide) which produce an electric field that is parallel to the transverse direction of the SiGe/Si stack in the rib waveguide structure.
  • FIG. 2 shows a general illustration of a phase shifter according to various embodiments.
  • the phase shifter may include rib waveguide 202.
  • the rib waveguide 202 may include a base 204.
  • the rib waveguide 202 may further include a stacked arrangement 206 on the base 204, the stacked arrangement 206 including alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the phase shifter may also include a first slab waveguide region
  • a first region of the rib waveguide 202, the first region of the rib waveguide 202 including a first region 204a of the base 204 and a first region 206a of the stacked arrangement 206, may be a doped region having a first type conductivity.
  • a second region of the rib waveguide 202 adjoining the first region of the rib waveguide 202, the second region of the rib waveguide 202 including a second region 204b of the base 204 and a second region 206b of the stacked arrangement 206, may be a doped region having a second type conductivity opposite to the first type conductivity.
  • the first slab waveguide region 208a, the first slab waveguide region 208a adjoining the first region 204a of the base 204 may be a doped region having the first type conductivity.
  • the second slab waveguide region 208b, the second slab waveguide region 208b adjoining the second region 204b of the base 204 may be a doped region having the second type conductivity.
  • the phase shifter may include a rib waveguide 202 which two lateral regions having opposite type conductivities.
  • the phase shifter may include a first slab waveguide region 208a adjoining a first lateral region of the rib waveguide 202 and having the same type conductivity as the first lateral region of the rib waveguide 202, as well as a second slab waveguide region 208b adjoining a second lateral region of the rib waveguide 202 and having the same type conductivity as the second lateral region of the rib waveguide 202.
  • FIG. 2 serves to illustrate some features of the phase shifter according to various embodiments, and does not seek to limit the dimensions, aspects ratios, shapes etc. of these features.
  • the stacked arrangement 206 may be a vertical stacked arrangement, and as mentioned above, may include alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the stacked arrangement 206 may include a first SiGe layer on the base 204, a first Si layer on the first SiGe layer, a second SiGe layer on the first Si layer, a second Si layer on the second SiGe layer and so on.
  • the base 204 may include silicon.
  • the base 204 may be formed from the silicon layer of a silicon-on-insulator (SOI) substrate.
  • a width of the stacked arrangement 206 may be smaller than a width of the base 204.
  • Each SiGe layer may be strained due to the presence of the adjoining Si layers.
  • a percentage composition of germanium in the layers of silicongermanium (SiGe) is selected from a range from 5% to 40%. Less germanium may be used as compared to conventional Quantum-Confined Stark Effect-based (QCSE) modulators.
  • QCSE Quantum-Confined Stark Effect-based
  • quantum barrier layers may be more than 70% germanium while pure Ge (or higher percentage concentration of germanium than percentage concentration of germanium used in the quantum barrier layers) may be used as strained quantum well layers.
  • the layers of silicon-germanium may have a same percentage composition of germanium. In various other embodiments, the layers of silicongermanium (SiGe) may have different percentage compositions of germanium.
  • the percentage composition of germanium in a silicon-germanium layer may be provided by Sii- x Ge x , where x indicates the ratio of germanium. For instance, a silicon-germanium layer with 40% germanium may be indicated by Sio.6Geo.4-
  • Each layer of the layers of silicon-germanium may have a thickness below a critical thickness limit so that it remains strained.
  • the critical thickness limit may be dependent on the germanium percentage concentration, for example the critical thickness of SiGe with 30% germanium is approximately 60 nm before strain relaxation sets in.
  • each layer of the layers of silicon-germanium (SiGe) may have a thickness selected from a range of between 5 nm to 40 nm (inclusive of both end values).
  • each layer of the layers of silicon (Si) may have a thickness selected from a range from 5 nm to 40 nm.
  • the phase shifter may include a first electrode in electrical connection with the first slab waveguide region 208a. In various embodiments, the phase shifter may include a second electrode in electrical connection with the second slab waveguide region 208b. In various embodiments, the phase shifter may be configured such that a voltage difference applied between the first electrode and the second electrode induces an electric field substantially parallel to a transverse direction of the stacked arrangement.
  • the first electrode and/or the second electrode may include any suitable conductive material, e.g. a metal such as aluminum.
  • the phase shifter may include a cladding such that the first electrode extends through the cladding to be in contact with the first slab waveguide region 208a, and the second electrode extends through the cladding to be in contact with the second slab waveguide region 208b.
  • the cladding may include any suitable dielectric such as silicon oxide.
  • the first region of the rib waveguide (i.e. the first region 204a of the base 204 and the first region 206a of the stacked arrangement 206) may have a doping concentration selected from a range from 1 x 10 16 cm' 3 to 1 x 10 18 cm' 3 .
  • the second region of the rib waveguide (i.e. the second region 204b of the base 204 and the second region 206b of the stacked arrangement 206) may have a doping concentration selected from a range from 1 x 10 16 cm' 3 to 1 x 10 18 cm' 3 .
  • the second region of the rib waveguide may be lateral to the first region of the rib waveguide.
  • the second region 204b of the base 204 may be lateral to the first region 204a of the base 204.
  • the second region 206b of the stacked arrangement 206 may be lateral to the first region 206a of the stacked arrangement 206.
  • the first slab waveguide region 208a may have a doping concentration selected from a range from 1 x 10 19 cm' 3 to 1 x IO 20 cm' 3 .
  • the second slab waveguide region 208b may have a doping concentration selected from a range from 1 x 10 19 cm' 3 to 1 x IO 20 cm' 3 .
  • the first slab waveguide region 208a may be lateral to the first region of the base 204a.
  • the second slab waveguide region 208b may be lateral to the second region of the base 204b.
  • the first type conductivity may be n-type and the second type conductivity may be p-type. In various other embodiments, the first type conductivity may be p-type and the second type conductivity may be n-type.
  • p-type conductivity may be caused by introducing dopants such as boron, aluminum, and/or gallium, while n-type conductivity may be caused by introducing dopants such as phosphorus, arsenic and/or antimony.
  • a thickness of the first slab waveguide region 208a and/or the second slab waveguide region 208b may be selected from a range from 50 nm to 150 nm, e.g. 70 nm.
  • a thickness of the first slab waveguide region 208a may be equal to or greater than a thickness of the base 204.
  • a thickness of the second slab waveguide region 208b may be equal to or greater than a thickness of the base 204.
  • a width of the stacked arrangement may be selected from a range from 400 nm to 600 nm, e.g. 500 nm.
  • the phase shifter may be configured to operate in reverse bias.
  • a depletion region may be formed which extends substantially perpendicularly to the stack arrangement direction or extends substantially perpendicularly to the transverse direction along the layers of Si and SiGe in the rib waveguide structure.
  • the electric field may be in parallel with the stack arrangement transverse direction or the transverse direction along the layers of Si and SiGe in the rib waveguide structure.
  • the electric field direction and the direction of the dopant interface are denoted in FIG. 2.
  • Various embodiments may relate to a modulator including a phase shifter as described herein.
  • Various embodiments may include a Mach-Zehnder modulator including a first arm (for providing a first optical path) and a second arm (for providing a second optical path).
  • the Mach-Zehnder modulator may include a phase shifter in one or both arms.
  • the phase shifter(s) may cause a phase shift between light traveling through the first arm and the second arm.
  • Various embodiments may provide a modulator with a spurious free dynamic range (SFDR) > 130 dBc. Hz 2/3 for enabling analog radio over fiber fronthaul (ARoF) link.
  • SFDR spurious free dynamic range
  • ARoF analog radio over fiber fronthaul
  • Various embodiments may operate using the electro-optic mechanism (free carrier plasma dispersion or FCPD).
  • the free carrier plasma dispersion may tune the refractive index by changing the free carrier concentration in the rib waveguide structure. This may provide phase modulation (slowing of the optical wave) which results in optical intensity change at the modulator output due to optical interference effects.
  • a change in the potential difference applied between the first electrode and the second electrode of the phase shifter may change the free carrier concentration in the rib waveguide, thereby changing the refractive index.
  • the change in refractive index may change the phase of the optical wave passing through the phase shifter present in an optical arm of a modulator, thereby changing an intensity of an resultant optical wave at an output of the modulator due to interference between the optical wave passing through the phase shifter in the optical arm and another optical wave passing through another optical arm of the modulator.
  • FIG. 3 A shows a general illustration of a method of forming a phase shifter according to various embodiments.
  • the method may include, in 302, forming a rib waveguide.
  • the rib waveguide may include a base, and a stacked arrangement on the base, the stacked arrangement including alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the method may also include, in 304, forming a first slab waveguide region.
  • the method may further include, in 306, forming a second slab waveguide region.
  • a first region of the rib waveguide, the first region of the rib waveguide including a first region of the base and a first region of the stacked arrangement, may be a doped region having a first type conductivity.
  • a second region of the rib waveguide adjoining the first region of the rib waveguide, the second region of the rib waveguide including a second region of the base and a second region of the stacked arrangement, is a doped region having a second type conductivity opposite to the first type conductivity.
  • the first slab waveguide region, the first slab waveguide region adjoining the first region of the base may be a doped region having the first type conductivity.
  • the second slab waveguide region, the second slab waveguide region adjoining the second region of the base may be a doped region having the second type conductivity.
  • Various embodiments may relate to a method of forming a phase shifter as described herein.
  • the various steps shown in FIG. 3 A are not intended to be in sequence. Exemplary processing sequences would be illustrated below.
  • forming the stacked arrangement may include forming a mask on a substrate, and alternating depositing silicon-germanium (SiGe) and silicon (Si) over a portion of the substrate exposed by the mask before removing the mask. There may be blanket deposition of the SiGe and Si over the substrate and the mask. However, with the removal of the mask, only the portion of the SiGe layers and the Si layers that is over the exposed portion of the substrate may remain, while the remaining portions of the SiGe layers and the Si layers over the mask may be removed together with the mask.
  • SiGe silicon-germanium
  • Si silicon
  • forming the stacked arrangement may include alternating depositing silicon-germanium (SiGe) and silicon (Si) on a substrate to form the alternate layers of silicon-germanium (SiGe) and silicon (Si), forming a mask over the alternate layers of silicon-germanium (SiGe) and silicon (Si), and removing portions of the alternate layers of alternate layers of silicon-germanium (SiGe) and silicon (Si) exposed through the mask.
  • Depositing the alternate layers of silicon-germanium (SiGe) and silicon (Si) may be carried out via a suitable deposition method such as chemical vapor deposition (CVD).
  • CVD chemical vapor deposition
  • the substrate e.g. a silicon-on-insulator (SOI) substrate
  • SOI silicon-on-insulator
  • the etching may be carried out via dry etching, wet etching or a combination of dry etching and wet etching.
  • An initial thickness of the silicon layer may be selected from a range from 100 nm to 300 nm, e.g. 220 nm.
  • a thickness of the silicon layer i.e. corresponding to an intended thickness of the first slab waveguide region and/or the second slab waveguide region
  • a thickness of the first slab waveguide region may be equal to or greater than a thickness of the base.
  • a thickness of the second slab waveguide region may be equal to or greater than a thickness of the base.
  • the first region of the rib waveguide, the second region of the rib waveguide, the first slab waveguide region and the second slab waveguide region may be implanted with dopants via separate steps (i.e. via separate ion implantation and masking steps). At least 4 implantation steps may be required to form the pn junction in the phase shifter.
  • forming the first region of the rib waveguide, the second region of the rib waveguide, the first slab waveguide region and the second slab waveguide region may include annealing to activate the implanted dopants.
  • the method may also include forming a first electrode in electrical connection with the first slab waveguide region. In various embodiments, the method may further include forming a second electrode in electrical connection with the second slab waveguide region.
  • the method may include forming a cladding.
  • the first electrode, the second electrode and the cladding may be formed after ion implantation.
  • a dielectric such as silicon oxide may be deposited over the rib waveguide, the first slab waveguide region and the second slab waveguide region to forming a cladding.
  • Portions of the cladding may be removed to form trenches (a first trench extending to the first slab waveguide region and a second trench extending to the second slab waveguide region), and a suitable electrically conductive material such as aluminum may be deposited in the trenches to form the first electrode and the second electrode.
  • FIG. 3B shows another illustration of a method of forming a phase shifter according to various embodiments.
  • the method may include, in 352, forming a slab waveguide.
  • the method may further include, in 354, depositing a stack of SiGe/Si layers to form a rib waveguide section.
  • the method may include, in 356, performing ion implantation to form at least 4 regions of different conductivity types and doping concentrations.
  • the method may also include, in 358, annealing the structure.
  • the method may additionally include, in 360, depositing the metal electrodes.
  • FIG. 4A shows a cross-sectional schematic of a phase shifter 400 according to various embodiments.
  • FIG. 4B shows a modulator in which the phase shifter 400 is arranged along one of the two optical arms of the modulator according to various embodiments. The two optical arms may be located at a distance from an optical source 450.
  • FIG. 4A corresponds to line A-A illustrated in FIG. 4B.
  • the phase shifter 400 may include rib waveguide 402 (alternatively referred as rib waveguide section).
  • the rib waveguide 402 may include or consist of a base 404 and a stacked arrangement 406 on the base 404, the stacked arrangement 406 including or consisting of alternate layers of silicon (Si) and layers of silicon-germanium (SiGe).
  • the phase shifter may also include a first slab waveguide region 408a and a second slab waveguide region 408b.
  • a first region of the rib waveguide 402, the first region of the rib waveguide 402 including or consisting of a first region 404a of the base 404 and a first region 406a of the stacked arrangement 406, may be a doped region having a first type conductivity.
  • a second region of the rib waveguide 402 adjoining (and lateral to) the first region of the rib waveguide 402, the second region of the rib waveguide 402 including or consisting of a second region 404b of the base 404 and a second region 406b of the stacked arrangement 406, may be a doped region having a second type conductivity opposite the first type conductivity.
  • the first slab waveguide region 408a, the first slab waveguide region 408a adjoining (and lateral to) the first region 404a of the base 404 may be a doped region having the first type conductivity.
  • the second slab waveguide region 408b, the second slab waveguide region 408b adjoining (and lateral to) the second region 404b of the base 404 may be a doped region having the second type conductivity.
  • the phase shifter 400 may also include a first electrode 410a in electrical connection with the first slab waveguide region 408a, and a second electrode 410b in electrical connection with the second slab waveguide region 408b.
  • the phase shifter may additionally include a cladding 412 such that the first electrode 410a extends through the cladding 412 to be in ohmic contact with the first slab waveguide region 408a, and the second electrode 410b extends through the cladding 412 to be in ohmic contact with the second slab waveguide region
  • optical signals at wavelengths near 1310 nm or 1550 nm which are suitable for communication applications may propagate in the rib waveguide 402.
  • the optical signals may be emitted or generated by the optical source 450.
  • the germanium (Ge) composition may be between 5% to 40% (inclusive of both end values).
  • the percentage compositions of Ge may be varied across different SiGe layers, while in various other embodiments, the SiGe layers may have the same percentage composition of Ge.
  • the thickness of each SiGe layer may be required to be within the critical thickness limit to avoid strain relaxation. In various embodiments, the thickness of each SiGe layer may be between 5 nm to 40 nm (inclusive of both end values). The thickness of each Si layer may be between 5 nm to 40 nm (inclusive of both end values).
  • the number of periods of alternate Si and SiGe layers may vary between 2 to 9 periods (inclusive of both end values).
  • the rib waveguide 402 may contain a first doped region (including a first region 404a of the base 404 and a first region 406a of the stacked arrangement 406) with a certain type conductivity, such as p-type, and a second doped region (including a second region 404b of the base 404 and a second region 406b of the stacked arrangement 406) with another type conductivity, such as n-type.
  • the doping concentrations in the rib waveguide may be between 1 x 10 16 cm -3 to 1 x 10 18 cm -3 (inclusive of both end values).
  • the dopant interface may substantially be perpendicular to the plane of Si/SiGe stack.
  • the slab waveguide regions 408a, 408b may each be the same type of conductivity as the adjacent doped region of the rib waveguide 402.
  • the doping concentrations of these slab waveguide regions 408a, 408b may be between 1 x 10 19 cm -3 to 1 x IO 20 cm -3 (inclusive of both end values).
  • the dopings may be contributed by dopants such as boron, aluminum, and/or gallium for p-type, and phosphorus, arsenic, and/or antimony for n-type.
  • the phase shifter 400 may be operated under reverse bias voltage.
  • the bias voltage signal and radio frequency modulation signal may be applied at the electrodes 410a, 410b which form the cathode nearer to a n-type slab waveguide region, and anode nearer to a p-type slab waveguide region.
  • the applied electric field may be parallel to the transverse direction of the Si/SiGe stack in the rib waveguide structure.
  • FIG. 4C shows a cross-sectional schematic of another phase shifter 400’ according to various embodiments.
  • the phase shifter 400’ has similar features as phase shifter 400 shown in FIG. 4A, and corresponding features are labelled with the same reference number.
  • the slab waveguide regions 408a, 408b of phase shifter 400’ may be thicker than the base 404.
  • the phase shifter 400’ may also include a further silicon layer having a region 404c of the first type conductivity and a region 404d of the second type conductivity on the stacked arrangement 406.
  • FIG. 4D shows a perspective view of the phase shifter 400’ according to various embodiments shown in FIG. 4C. Corresponding features are labelled with the same reference number.
  • FIGS. 5A-G illustrate a method of fabricating the phase shifter according to various embodiments.
  • FIG. 5A shows a top silicon (Si) layer 514 of a silicon-on-insulator (SOI) substrate according to various embodiments.
  • the initial thickness of the silicon layer 514 of the SOI substrate may be of any value from 100 nm to 300 nm, e.g. 220 nm.
  • the silicon layer 514 may be first etched to the intended slab waveguide thickness.
  • the intended slab waveguide thickness may be of any value from 50 nm to 150 nm, e.g. 70 nm.
  • the etching may be dry etching, wet etching or a combination of wet etching and dry etching to achieve a smooth surface suitable for deposition.
  • FIG. 5B shows the silicon (Si) layer 514’ after etching according to various embodiments.
  • FIG. 5C shows the patterning of the silicon oxide layer 516 to form the trench 518 according to various embodiments. Silicon oxide may be deposited onto the etched Si layer 514’ to form a silicon oxide layer 516. Atrench 518 may be subsequently etched onto the silicon oxide layer 516 using photoresist for pattern definition. The photoresist may be removed at this point.
  • FIG. 5D shows the formation of the stacked arrangement 506 of the rib waveguide according to various embodiments.
  • the silicon oxide layer 516 with the trench 518 may be used as a mask.
  • a silicon-germanium (SiGe) layer may be deposited directly in the trench 518 onto the exposed Si layer 514’. Once the SiGe layer is of sufficient thickness, a Si layer may be deposited. The alternating SiGe and Si deposition steps may be performed until a sufficient thickness is achieved to form the stacked arrangement 506 of the rib waveguide. There may be blanket deposition of the SiGe and Si over the silicon oxide layer 516 and the mask.
  • SiGe silicon-germanium
  • the width of the trench may define the width of the stacked arrangement 506.
  • the width of the stacked arrangement 506 may be between 400 nm to 600 nm (inclusive of both end values), e.g. 500 nm.
  • the surrounding silicon oxide layer 516 may now be removed.
  • FIG. 5E shows the formation of doped regions in the rib waveguide and doped slab waveguide regions according to various embodiments. Ion implantation may be used to form the doped regions in the rib waveguide and to form doped slab waveguide regions. Each region of different conductivities and doping concentrations may first be defined using photoresist as masking layer, and ion implantation using suitable conditions may then be carried out. A minimum of four of such steps is required to form the following four regions: (i) a first region of the rib waveguide including a first region 506a of the stacked arrangement 506 and a first region 504a of the base 504; (ii) a second region of the rib waveguide including a second region
  • a cladding 512 (also referred to as upper cladding layer) of silicon oxide may then be deposited.
  • FIG. 5F shows forming of the cladding 512 according to various embodiments.
  • FIG. 5G shows the forming of the electrodes 510a, 510b according to various embodiments.
  • trenches may be etched into the cladding 512 until reaching the first slab waveguide region 508a and the second slab waveguide region 508b, and a metal such as aluminum may be deposited into the trenches to form the electrodes 510a, 510b.
  • FIGS. 6A-F illustrate a method of fabricating the phase shifter according to various other embodiments.
  • a silicon-germanium (SiGe) layer may be deposited directly onto the exposed Si layer 614’ (corresponding to Si layer 514’ shown in FIG. 5B). Once the SiGe layer is of sufficient thickness, a Si layer may be deposited. The alternating SiGe and Si deposition steps may be performed until a sufficient thickness is achieved, thereby forming stack 606’.
  • FIG. 6A shows the formation of stack 606’ according to various embodiments.
  • FIG. 6D shows the formation of doped regions in the rib waveguide and doped slab waveguide regions according to various embodiments. Ion implantation may be used to form the doped regions in the rib waveguide and to form doped slab waveguide regions. Each region of different conductivities and doping concentrations may first be defined using photoresist as masking layer, and ion implantation using suitable conditions may then be carried out.
  • a minimum of four of such steps is required to form the following four regions: (i) a first region of the rib waveguide including a first region 606a of the stacked arrangement 606 and a first region 604a of the base 604; (ii) a second region of the rib waveguide including a second region 606b of the stacked arrangement 606 and a second region 604b of the base 604; (iii) a first slab waveguide region 608a; and (iv) a second slab waveguide region 608b.
  • An annealing step may then be used to activate the implanted dopants. Any remaining oxide or photoresist may be removed after the ion implantation step.
  • the ion implantation and annealing steps may be carried out before the patterning steps as shown in FIGS. 6B-C.
  • the portions of the stack 606’ over the portions of the silicon layer 614’ used to define slab waveguide regions 608a and 608b may be implanted with ions of the same type conductivity as that used for doping slab waveguide regions 608a and 608b, respectively. These portions of the stack 606’ over slab waveguide regions 608a and 608b may subsequently be etched away as shown in FIGS. 6B-C.
  • a cladding 612 (also referred to as upper cladding layer) of silicon oxide may then be deposited.
  • FIG. 6E shows forming of the cladding 612 according to various embodiments.
  • FIG. 6F shows the forming of the electrodes 610a, 610b according to various embodiments.
  • trenches may be etched into the cladding 612 until reaching the silicon layer 614’, and a metal such as aluminum may be deposited into the trenches to form the electrodes 610a, 610b.
  • FIG. 7 shows (top) a plot of thickness (in nanometers or nm) as a function of number of periods illustrating the variation of spurious free dynamic range (SFDR) (decibels relative to carrier Hertz to power of two-thirds or dBc. Hz 2/3 ) for Sio.gGeo.i according to various embodiments; (middle) a plot of thickness (in nanometers or nm) as a function of number of periods illustrating the variation of spurious free dynamic range (SFDR) (decibels relative to carrier Hertz to power of two-thirds or dBc.
  • SFDR spurious free dynamic range
  • each plot may represent a structure of a particular Ge composition.
  • the largest spurious free dynamic range obtained for each Ge composition at 10%, 20% and 30% are 132.4 dBc. Hz 2/3 , 143.5 dBc. Hz 2/3 and 133.3 dBc.
  • Hz 2/3 respectively, interestingly for 5 periods, 15 nm thick SiGe and Si. It is demonstrated that a number of design variation may achieve SFDR > 130 dBc. Hz 2/3 and the best simulated SFDR is 143.5 dBc. Hz 2/3 .
  • the design space is large and may be constrained by number of periods of Si/Sii- x Ge x , thickness of Sii- x Ge x layers, composition of Sii- x Ge x , and phase shifter length.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Nonlinear Science (AREA)
  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)

Abstract

Divers modes de réalisation peuvent concerner un déphaseur. Le déphaseur peut comprendre un guide d'ondes à nervure. Le guide d'ondes à nervure peut comprendre une base et un agencement empilé sur la base, l'agencement empilé comprenant des couches de silicium (Si) et des couches de silicium-germanium (SiGe) alternées. Le déphaseur peut également comprendre une première région de guide d'ondes en plaque et une seconde région de guide d'ondes en plaque. Une première région du guide d'ondes à nervure, la première région du guide d'ondes à nervure comprenant une première région de la base et une première région de l'agencement empilé, peut être une région dopée ayant une conductivité de premier type. Une seconde région du guide d'ondes à nervure adjacente à la première région du guide d'ondes à nervure, la seconde région du guide d'ondes à nervure comprenant une seconde région de la base et une seconde région de l'agencement empilé, peut être une région dopée ayant une conductivité de second type.
PCT/SG2023/050578 2023-08-22 2023-08-22 Déphaseur et son procédé de formation WO2025042329A1 (fr)

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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20180024410A1 (en) * 2015-02-06 2018-01-25 Photonics Electronics Technology Reserach Association Optical modulator and method of manufacturing same
US20200073153A1 (en) * 2018-08-31 2020-03-05 Stmicroelectronics (Crolles 2) Sas Electro-Optical Modulator and Methods of Formation Thereof
US20230229029A1 (en) * 2022-01-20 2023-07-20 Industry-University Cooperation Foundation Hanyang University Erica Campus Optical phase shifter having l-shaped pn junction and manufacturing method therefor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20180024410A1 (en) * 2015-02-06 2018-01-25 Photonics Electronics Technology Reserach Association Optical modulator and method of manufacturing same
US20200073153A1 (en) * 2018-08-31 2020-03-05 Stmicroelectronics (Crolles 2) Sas Electro-Optical Modulator and Methods of Formation Thereof
US20230229029A1 (en) * 2022-01-20 2023-07-20 Industry-University Cooperation Foundation Hanyang University Erica Campus Optical phase shifter having l-shaped pn junction and manufacturing method therefor

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
KUO, Y. H. ET AL.: "Quantum-Confined Stark Effect in Ge/SiGe Quantum Wells on Si for Optical Modulators", IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, vol. 12, no. 6, 31 December 2006 (2006-12-31), pages 1503 - 1513, XP011151841, [retrieved on 20240228], DOI: 10.1109/JSTQE.2006.883146 *

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