WO2000007049A1 - Optical waveguide component - Google Patents

Optical waveguide component Download PDF

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Publication number
WO2000007049A1
WO2000007049A1 PCT/EP1999/004040 EP9904040W WO0007049A1 WO 2000007049 A1 WO2000007049 A1 WO 2000007049A1 EP 9904040 W EP9904040 W EP 9904040W WO 0007049 A1 WO0007049 A1 WO 0007049A1
Authority
WO
WIPO (PCT)
Prior art keywords
refractive index
core
substrate
cladding layer
layer
Prior art date
Application number
PCT/EP1999/004040
Other languages
French (fr)
Inventor
Tsjerk Hans Hoekstra
Original Assignee
Akzo Nobel N.V.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Akzo Nobel N.V. filed Critical Akzo Nobel N.V.
Priority to JP2000562783A priority Critical patent/JP2002521731A/en
Priority to EP99926522A priority patent/EP1018042A1/en
Priority to CA002304200A priority patent/CA2304200C/en
Publication of WO2000007049A1 publication Critical patent/WO2000007049A1/en
Priority to US09/538,594 priority patent/US6408126B1/en

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Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light 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
    • G02B6/122Basic optical elements, e.g. light-guiding paths
    • G02B6/125Bends, branchings or intersections
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12Light 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
    • G02B2006/12083Constructional arrangements
    • G02B2006/12097Ridge, rib or the like

Definitions

  • the invention pertains to an optical waveguide component comprising a substrate, a core-matching refractive index lower cladding layer, a core layer, a core-matching refractive index upper cladding layer, and a low refractive index top cladding.
  • Such a component is known from, e.g., International patent application WO 97/01782.
  • This publication concerns optical components having an at least penta-layered polymer structure on a substrate comprising: a) a low refractive index bottom cladding layer, b) a core-matching refractive index lower cladding layer, c) a core layer, d) a core-matching refractive index upper cladding layer, and e) a low refractive index top cladding layer.
  • slab modes, quasi- guided modes and/or scattered light (sometimes also referred to as radiation modes and stray light respectively) become trapped between the lower and upper cladding layers, with the core layer and the core-matching refractive index cladding layers serving as a (composite) core.
  • the core layer and the core-matching refractive index cladding layers serving as a (composite) core.
  • the said modes cannot have any interaction with the guide mode(s) in the core layer and a decrease of the optical performance is avoided.
  • avoiding interaction between a guided mode in the core layer and slab modes, quasi- guided modes and/scattered light will result in a considerably improved isolation (defined as the ratio of the optical power in an output in the on- state and the optical power in an output in the off-state).
  • Capture and/or absorption of the guided mode should preferably be smaller than 0.01 dB/cm, more preferably smaller than 0.001 dB/cm.
  • Leaking of slab modes, quasi-guided modes and/or scattered light to the substrate can be achieved by using a substrate that has a refractive index higher than that of the core-matching refractive index lower cladding layer and/or that functions as an absorber of the said undesirable modes.
  • a substrate that has a refractive index higher than that of the core-matching refractive index lower cladding layer and/or that functions as an absorber of the said undesirable modes.
  • Any material that absorbs and dissipates light in the optical frequencies used in the structure in question will do.
  • suitable materials are metals such as titanium, silver, gold, or nickel or non-transparent dielectric polymers containing a dye.
  • the substrate may comprise one or more (usually very thin) top layers or coatings, e.g., to promote adhesion to the core-matching refractive index lower cladding layer.
  • EP 642 052 discloses a polymeric thermo-optical device comprising a polymeric core layer sandwiched between two cladding layers having a refractive index lower than that of the guiding layer. A heating element is placed against one of the cladding layers and this layer has a lower refractive index than the other cladding layer.
  • the lower cladding layer is made up of two sublayers to provide optical isolation from the substrate.
  • the component is a thermo-optical component and/or the thickness of the core-matching refractive index lower cladding layer is (preferably at least 30 percent) greater than the thickness of the stack containing the core layer, the core-matching refractive index upper cladding layer, and the low refractive index upper cladding.
  • the core layer is asymmetrically buried in the layer stack, close to the heater element and far from the heatsink, i.e. the substrate.
  • the refractive index of the substrate is advantageous to select the refractive index of the substrate to be higher than the refractive index of the core-matching refractive index lower cladding layer.
  • Silicon substrates are preferably used, because silicon exhibits a very high refractive index and silicon substrates are readily available on the market and of homogeneous thickness. Furthermore, they are frequently used in integrated circuit techniques and apparatus.
  • thermo-optical components such as 1xN switches, switch matrices, and MZIs
  • Active optical components can be, e.g., so-called thermo-optical (TO) components, which are preferred, or electro-optical components (EO). Both thermo-optical and electro-optical components are known.
  • thermo-optical components are based on the phenomenon of the optical waveguide material employed exhibiting a temperature dependent refractive index.
  • heating elements are provided (usually metal strips) to heat the polymeric cladding and core materials, in order to change the refractive index for switching.
  • the working of electro-optical devices is based on the phenomenon of the non-linear optically active material employed exhibiting an electric field dependent refractive index.
  • On top of the upper cladding layer electrodes are provided to apply an electric field to the non-linear optically active material to change the refractive index for switching.
  • Devices according to the invention can be used with advantage in optical communications networks of various kinds.
  • the optical components either will be directly combined with optical components such as light sources (laser diodes) or detectors, or they will be coupled to input and output optical fibres, usually glass fibres.
  • Polymer optical devices are commonly optical fibre-compatible and based on embedded or embedded ridge-type channel waveguides.
  • the resulting structure comprises a high refractive index core polymer (usually of rectangular or square cross-section) embedded in a lower refractive index cladding material.
  • Suitable materials for and configurations of the cladding and the core layers are disclosed, int. al., in M.B.J. Diemeer et al., "Polymeric phased array wavelength multiplexer operating around 1550 nm," Electronics Letters,
  • core-matching refractive index means that the refractive index is matched to that of the core so as to obtain the required contrast.
  • Figure 1 shows a polymeric five- or penta-layered structure on a silicon substrate in accordance with the prior art.
  • Figure 2 shows a polymeric four- layered structure on a silicon substrate in accordance with the present invention (in both structures N 0 eguals 1.513). Both devices were operated using light having a wavelength of 1550 nm and, in comparison with the one according to Figure 1 , the scattered light in the device according to the present invention was considerably reduced.

Abstract

The invention pertains to an optical waveguide component comprising a substrate, a core-matching refractive index lower cladding layer, a core layer, a core-matching refractive index upper cladding layer, a low refractive index upper cladding, wherein the core-matching refractive index lower cladding layer is deposited directly onto the substrate and has a thickness sufficient to avoid substantial capture and/or absorption by the substrate of a guided mode in the core layer, whereas slab modes, quasi-guided modes and/scattered light leak to the substrate. The components according to the invention allow high switching speeds and high confinement of a guided mode on the one hand and, on the other hand, absorption by the substrate of stray-light and radiation modes, which, in turn, leads to improved optical devices, such as optical switches with improved isolation.

Description

Optical waveguide component.
The invention pertains to an optical waveguide component comprising a substrate, a core-matching refractive index lower cladding layer, a core layer, a core-matching refractive index upper cladding layer, and a low refractive index top cladding.
Such a component is known from, e.g., International patent application WO 97/01782. This publication concerns optical components having an at least penta-layered polymer structure on a substrate comprising: a) a low refractive index bottom cladding layer, b) a core-matching refractive index lower cladding layer, c) a core layer, d) a core-matching refractive index upper cladding layer, and e) a low refractive index top cladding layer.
With this specific layer structure optimum confinement in the direction of the thickness of the stack of layers (also denoted as transverse direction) can be obtained, which results in less loss of light and an improved switching efficiency. However, present and future applications of optical devices require crosstalk to be as low as possible.
Accordingly, it is an object of the present invention to further reduce crosstalk. This is achieved, in the components described in the first paragraph, by leaving out the low refractive index bottom cladding layer and employing a single core-matching refractive index lower cladding layer which has a thickness sufficient to avoid substantial capture and/or absorption by the substrate of a guided mode in the core layer, whereas slab modes, quasi-guided modes and/scattered light leak to the substrate.
It was found that, in the said penta-layered components, slab modes, quasi- guided modes and/or scattered light (sometimes also referred to as radiation modes and stray light respectively) become trapped between the lower and upper cladding layers, with the core layer and the core-matching refractive index cladding layers serving as a (composite) core. By leaving out the bottom cladding layer, making sure that the slab modes, quasi- guided modes and/scattered light leak to the substrate, and selecting the thickness of the core-matching refractive index lower cladding layer such that substantial absorption of a guided mode by the substrate is avoided, crosstalk and other detrimental phenomena are significantly reduced. Once captured or absorbed by the substrate, the said modes cannot have any interaction with the guide mode(s) in the core layer and a decrease of the optical performance is avoided. E.g., for an 1x2 optical switch, avoiding interaction between a guided mode in the core layer and slab modes, quasi- guided modes and/scattered light will result in a considerably improved isolation (defined as the ratio of the optical power in an output in the on- state and the optical power in an output in the off-state).
Capture and/or absorption of the guided mode should preferably be smaller than 0.01 dB/cm, more preferably smaller than 0.001 dB/cm.
Leaking of slab modes, quasi-guided modes and/or scattered light to the substrate can be achieved by using a substrate that has a refractive index higher than that of the core-matching refractive index lower cladding layer and/or that functions as an absorber of the said undesirable modes. Any material that absorbs and dissipates light in the optical frequencies used in the structure in question will do. Examples of suitable materials are metals such as titanium, silver, gold, or nickel or non-transparent dielectric polymers containing a dye. It is noted that the substrate may comprise one or more (usually very thin) top layers or coatings, e.g., to promote adhesion to the core-matching refractive index lower cladding layer.
The components according to the invention allow high switching speeds and high confinement of a guided mode, require less power for switching and, due to the capture or absorption by the substrate of slab modes, quasi- guided modes and/or scattered light, exhibit less crosstalk. It is noted that EP 642 052 discloses a polymeric thermo-optical device comprising a polymeric core layer sandwiched between two cladding layers having a refractive index lower than that of the guiding layer. A heating element is placed against one of the cladding layers and this layer has a lower refractive index than the other cladding layer. In a particularly preferred embodiment, the lower cladding layer is made up of two sublayers to provide optical isolation from the substrate. Thus, the gist of EP 642 052 runs counter to that of the present invention.
In a preferred embodiment, the component is a thermo-optical component and/or the thickness of the core-matching refractive index lower cladding layer is (preferably at least 30 percent) greater than the thickness of the stack containing the core layer, the core-matching refractive index upper cladding layer, and the low refractive index upper cladding. Thus, the core layer is asymmetrically buried in the layer stack, close to the heater element and far from the heatsink, i.e. the substrate.
As will be clear from the above explanations, it is advantageous to select the refractive index of the substrate to be higher than the refractive index of the core-matching refractive index lower cladding layer. Silicon substrates are preferably used, because silicon exhibits a very high refractive index and silicon substrates are readily available on the market and of homogeneous thickness. Furthermore, they are frequently used in integrated circuit techniques and apparatus.
Within the framework of the present invention, components wherein the layers are made of optical polymeric materials are preferred. Active optical components, such as 1xN switches, switch matrices, and MZIs, can be, e.g., so-called thermo-optical (TO) components, which are preferred, or electro-optical components (EO). Both thermo-optical and electro-optical components are known. The working of thermo-optical components is based on the phenomenon of the optical waveguide material employed exhibiting a temperature dependent refractive index. On top of the upper cladding layer heating elements are provided (usually metal strips) to heat the polymeric cladding and core materials, in order to change the refractive index for switching.
The working of electro-optical devices is based on the phenomenon of the non-linear optically active material employed exhibiting an electric field dependent refractive index. On top of the upper cladding layer electrodes are provided to apply an electric field to the non-linear optically active material to change the refractive index for switching.
Of course, the invention also applies to passive components, like splitters and combiners.
Devices according to the invention can be used with advantage in optical communications networks of various kinds. Generally, the optical components either will be directly combined with optical components such as light sources (laser diodes) or detectors, or they will be coupled to input and output optical fibres, usually glass fibres.
Polymer optical devices are commonly optical fibre-compatible and based on embedded or embedded ridge-type channel waveguides. The resulting structure comprises a high refractive index core polymer (usually of rectangular or square cross-section) embedded in a lower refractive index cladding material.
Suitable materials for and configurations of the cladding and the core layers are disclosed, int. al., in M.B.J. Diemeer et al., "Polymeric phased array wavelength multiplexer operating around 1550 nm," Electronics Letters,
Vol. 32 (1996), pp. 1132-1133; and T.A. Tumolillo et al., "Solid State Optical Space Switches for Network Cross-Connect and Protection Applications," IEEE Communications Magazine (1997), pp 124-130; and International Patent Application WO 97/01782.
Within the framework of the present invention the term "core-matching refractive index" means that the refractive index is matched to that of the core so as to obtain the required contrast.
Figure 1 shows a polymeric five- or penta-layered structure on a silicon substrate in accordance with the prior art. Figure 2 shows a polymeric four- layered structure on a silicon substrate in accordance with the present invention (in both structures N0 eguals 1.513). Both devices were operated using light having a wavelength of 1550 nm and, in comparison with the one according to Figure 1 , the scattered light in the device according to the present invention was considerably reduced.

Claims

Claims
1. An optical waveguide component comprising a substrate, a core- matching refractive index lower cladding layer, a core layer, a core- matching refractive index upper cladding layer, and a low refractive index top cladding, characterised in that the core-matching refractive index lower cladding layer is deposited directly onto the substrate and has a thickness sufficient to avoid substantial capture and/or absorption by the substrate of a guided mode in the core layer, whereas slab modes, quasi-guided modes and/or scattered light leak to the substrate.
2. The optical waveguide component according to claim 1 wherein the component is a thermo-optical component.
3. The optical waveguide component according to claim 1 or 2 wherein the thickness of the core-matching refractive index lower cladding layer is greater than the thickness of the stack containing the core layer, the core- matching refractive index upper cladding layer, and the low refractive index upper cladding.
4. The optical waveguide component according to claim 3 wherein the thickness of the core-matching refractive index lower cladding layer is at least 30 percent greater than the thickness of the said stack.
5. The optical waveguide component according to any one of the preceding claims wherein the layers are made of polymeric materials.
6. The optical waveguide component according to any one of the preceding claims wherein the component comprises a switch.
PCT/EP1999/004040 1998-07-24 1999-06-09 Optical waveguide component WO2000007049A1 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP2000562783A JP2002521731A (en) 1998-07-24 1999-06-09 Optical waveguide device
EP99926522A EP1018042A1 (en) 1998-07-24 1999-06-09 Optical waveguide component
CA002304200A CA2304200C (en) 1998-07-24 1999-06-09 Optical waveguide component
US09/538,594 US6408126B1 (en) 1998-07-24 2000-03-24 Optical waveguide component

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
EP98202496 1998-07-24
EP98202496.0 1998-07-24

Related Child Applications (1)

Application Number Title Priority Date Filing Date
US09/538,594 Continuation-In-Part US6408126B1 (en) 1998-07-24 2000-03-24 Optical waveguide component

Publications (1)

Publication Number Publication Date
WO2000007049A1 true WO2000007049A1 (en) 2000-02-10

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PCT/EP1999/004040 WO2000007049A1 (en) 1998-07-24 1999-06-09 Optical waveguide component

Country Status (5)

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US (1) US6408126B1 (en)
EP (1) EP1018042A1 (en)
JP (1) JP2002521731A (en)
CA (1) CA2304200C (en)
WO (1) WO2000007049A1 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20020018636A1 (en) * 2000-08-02 2002-02-14 Gemfire Corporation Device and method for variable attenuation of an optical channel
US8098968B2 (en) * 2007-09-04 2012-01-17 International Business Machines Corporation Silicide thermal heaters for silicon-on-insulator nanophotonic devices
WO2015108529A1 (en) * 2014-01-17 2015-07-23 Empire Technology Development Llc Optical fibers without cladding
US9453967B2 (en) * 2014-10-17 2016-09-27 Lumentum Operations Llc High power misalignment-tolerant fiber assembly
US10620371B2 (en) * 2016-03-05 2020-04-14 Huawei Technologies Canada Co., Ltd. Waveguide crossing having rib waveguides

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0642052A1 (en) * 1993-08-24 1995-03-08 Akzo Nobel N.V. Polymeric thermo-optical waveguide device
WO1997001782A1 (en) * 1995-06-28 1997-01-16 Akzo Nobel N.V. At least penta-layered optical device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5633966A (en) * 1995-04-07 1997-05-27 Sumitomo Electric Industries, Ltd. Method of forming refractive index distribution in light transmission path, and optical filter and method of using the same
EP0961139B1 (en) * 1997-02-19 2006-12-13 Opnext Japan, Inc. Polymer optical waveguide, optica integrated circuit , optical module and optical communication apparatus

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0642052A1 (en) * 1993-08-24 1995-03-08 Akzo Nobel N.V. Polymeric thermo-optical waveguide device
WO1997001782A1 (en) * 1995-06-28 1997-01-16 Akzo Nobel N.V. At least penta-layered optical device

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Publication number Publication date
CA2304200C (en) 2006-10-17
US6408126B1 (en) 2002-06-18
EP1018042A1 (en) 2000-07-12
CA2304200A1 (en) 2000-02-10
JP2002521731A (en) 2002-07-16

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