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EP0963395A1 - Polymers comprising a fluorinated carbonate moiety - Google Patents

Polymers comprising a fluorinated carbonate moiety

Info

Publication number
EP0963395A1
EP0963395A1 EP98909428A EP98909428A EP0963395A1 EP 0963395 A1 EP0963395 A1 EP 0963395A1 EP 98909428 A EP98909428 A EP 98909428A EP 98909428 A EP98909428 A EP 98909428A EP 0963395 A1 EP0963395 A1 EP 0963395A1
Authority
EP
European Patent Office
Prior art keywords
refractive index
polymer
cladding layer
core
alkyl
Prior art date
Legal status (The legal status 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 status listed.)
Withdrawn
Application number
EP98909428A
Other languages
German (de)
French (fr)
Inventor
Richard Herman Woudenberg
Tjerk Oedse Boonstra
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
JDS UNIPHASE Inc
Original Assignee
Akzo Nobel NV
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 NV filed Critical Akzo Nobel NV
Priority to EP98909428A priority Critical patent/EP0963395A1/en
Priority claimed from PCT/EP1998/000717 external-priority patent/WO1998038237A1/en
Publication of EP0963395A1 publication Critical patent/EP0963395A1/en
Withdrawn legal-status Critical Current

Links

Definitions

  • optical components are meant here, thermo-optical components, electro-optical components or passive components.
  • 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.
  • Polymeric thermo-optical components generally comprise a polymeric three-layer structure on a substrate.
  • the three-layer structure comprises a low refractive index lower cladding layer, a high refractive index core layer, and a low refractive index upper cladding layer.
  • heating elements are provided (usually metal strips) to heat the polymeric cladding and core material, 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.
  • Polymeric electro-optical components in general also comprise a polymeric three-layer structure.
  • the three-layer structure comprises a low refractive index lower cladding layer, a non-linear optically active, high refractive index core layer, and a low refractive index upper cladding layer.
  • 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.
  • Optical components having an at least penta-layered polymer structure on a substrate comprising: a) a low refractive index lower 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 upper cladding layer, are also known in the art.
  • silicon substrates are used for optical components. These substrates are readily available on the market and are of homogeneous thickness. Furthermore, they are frequently used in integrated circuit techniques and apparatus.
  • One disadvantage of silicon is its high refractive index. Due to this high refractive index the light of the propagating mode might leak into the silicon substrate.
  • the low refractive index lower cladding layer a) is applied to prevent leaking of light from the propagating mode into the silicon substrate.
  • the low refractive index lower cladding a) is also of advantage in controlling the confinement of the propagating mode. Using a low refractive index lower cladding a) of appropriate index and thickness gives ample freedom in designing the core-matching refractive index cladding layers b) and d) and the core layer c).
  • the optical components usually comprise metal electrodes on top of the upper cladding layer, either for use as heating elements or for applying an electric field.
  • These electrodes are usually made of gold and/or other metals such as chromium, nickel, copper, platinum, or combinations or alloys thereof.
  • the low refractive index upper cladding e) is applied to prevent leaking of the light from the propagating mode into the attenuating (gold) electrodes.
  • the refractive indices of the low refractive index lower and upper cladding layers a) and e) are usually (approximately) the same.
  • Employing a low refractive index upper cladding layer e) with a larger thickness than that of the low refractive index lower cladding layer a) makes it possible to use a core-matching refractive index upper cladding layer d) which is thinner than the core-matching refractive index lower cladding b).
  • the resulting combined thickness of the low refractive index upper cladding d) and the core-matching refractive index upper cladding e) is smaller than the combined thickness of the low refractive index lower cladding a) and the core-matching refractive index lower cladding b).
  • the structure is transversally asymmetric, with the core layer being close to the electrodes and thus experiencing stronger induced thermo-optical or electro-optical effects, resulting in a more efficient component.
  • the core-matching refractive index lower cladding b) and the core- matching refractive index upper cladding d) are applied to obtain transversal confinement of the propagating mode.
  • the refractive index can be chosen in a relatively wide range to achieve the required properties, such as: monomode behavior, good overlap with a Standard Single Mode Fiber (SMF).
  • SMF Standard Single Mode Fiber
  • Lateral confinement can be achieved by all known methods for defining channels in planar waveguiding components. Suitable methods are:
  • the refractive index of the core-matching refractive index cladding layers b) and d) should be adapted to the refractive index of the bleached parts of the core.
  • the refractive index of the core-matching refractive index upper cladding layer material is chosen such as to give the required properties, such as: monomode behavior, good overlap with a Standard Single Mode Fiber (SMF), low polarization dependence, low bend losses.
  • SMF Standard Single Mode Fiber
  • thermo-optical devices are so-called optical polymers. Many optical polymers are known in the art, but there is still need for improvement.
  • a particular problem of polymeric waveguides is the difference between the refractive indices of the core layer and the surrounding cladding layers. Typically, these index differences are in the range of 0.003 to 0.008.
  • switching is induced by index differences of 0.001 (digital switches) to 0.0001 (interferometer switches). These small index differences can be induced by thermo- or electro-optical properties of polymeric materials.
  • the core index is lowered by locally heating the layer stack by means of a heating element.
  • this material must have a low absorption at the operating wavelengths (1.3 and 1.5 ⁇ m). It is therefore an object of the invention to provide polymeric material with very low refractive index, and very low optical loss, preferably less than 0.15 dB/cm.
  • the polymeric material must also display high Tg because of chemical and optical stability, and be cross-linkable to obtain cladding layers suitable for thermo-optical waveguides.
  • polymeric material when polymeric material is used as a waveguide core, it is advantageous to use material with an index similar to that of the optical fiber attached to said waveguide, which effective index for standard single mode fiber is 1.467 at 1.3 ⁇ m and 1.468 at 1.5 ⁇ m.
  • doped silica is used as a core, the polymers of the invention can be used advantageously as cladding because their refractive indices can be lower than that of the glass core, which has the advantage that these hybrid waveguides can be rendered athermal.
  • optical polymers or NLO polymers are rendered cross-linkable either by the incorporation of cross-linkable monomers or by mixing cross-linkers such as polyisocyanates, polyepoxides, etc. into the polymer.
  • the polymer further comprises a cross-linkable moiety derived from a diol selected from:
  • A, A ⁇ and A 2 are independently a bond or C 1-12 alkylene, or together with the carbon atoms to which they are bonded form a 5- or 6-membered ring;
  • B is independently O or C 1-4 alkyl
  • D is H or C ⁇ alkyl
  • E is C 1-6 alkylidene; and each of the alkyl, alkylene, and alkylidene groups may be halogenated.
  • C ⁇ alkyl means an alkyl group with 1 to 4 carbon atoms, such as methyl, ethyl, propyl, isopropyl, butyl, terf-butyl, and the like. Methyl is the preferred alkyl group.
  • C 1-12 alkylene means an alkylene group with 1 to 12 carbon atoms, such as methylene, ethylene, propylene, 2,2,-dimethylpropylene, dodecylene, and the like.
  • A, A-,, and A 2 are preferably a bond or an alkylene group with 1-3 carbon atoms.
  • C ⁇ 6 alkylidene means an alkylidene group with 1 to 6 carbon atoms, such as methylene, ethylidene, propylidene, 2-methylpropylidene, and the like. Methylene and ethylidene are the preferred alkylidene groups.
  • alkyl, alkylene, or alkylidene groups are halogenated, chlorine and fluorine are the preferred halogens. Fluorine is the most preferred halogen.
  • the index of the polymer can be fine-tuned by selecting the number, the type, and the combination of halogens.
  • the polymer of the invention can be prepared by standard methods known in the art for the preparation of similar polymers.
  • the bischloroformate of hexafluorobisphenol A or hexafluoroisopropylidene- dicyclohexanediol bischloroformate can be polymerized in suitable solvents with the hexafluoro-perhydro-bisphenol A, the synthesis of which has been disclosed in EP 0,279,462, optionally in the presence of suitable cross- linkable moieties, such as the above-mentioned diols.
  • Non-linear electric polarization may give rise to several optically non-linear phenomena, such as frequency doubling, Pockels effect, and Kerr effect.
  • the groups present in the polymer usually hyperpolarizable side-groups, first have to be aligned (poled). Such alignment is commonly effected by exposing the polymeric material to electric (DC) voltage, the so-called poling field, with such heating as will render the polymeric chains sufficiently mobile for orientation.
  • DC electric
  • oxygen scavengers and radical scavengers and the like may be added to the optical polymers.
  • the invention is further illustrated by the following examples. EXAMPLE I
  • Hexafluoro-perhydro-bisphenol A (150.0 g), hexafluorobisphenol A bischloroformate (398.7 g), and 2,3-dihydroxypropyl methacrylate (68.9 g) were dissolved in a mixture of anhydrous dichloromethane (1.5 I) and anhydrous tetrahydrofuran (1 I). After cooling to 0°C, anhydrous pyridine (133.4 g) was added dropwise. After the addition, the reaction mixture was allowed to warm to room temperature and stirred overnight. The pyridine hydrochloride was filtered off and the filtrate was precipitated in 50 I of methanol. The precipitate was filtered off and washed with methanol. The polymer was dried overnight in vacuo at 5 kPa at 50°C. Yield 460 g. Mw 26,000; Mn 13,000; Tg 119-126°C; TGA 190°C.
  • the polymer of the invention has a Tg and an optical loss which are comparable with those of higher refractive index materials, whereas the Tg of the polymer of the invention is substantially higher than the Tg of other very low refractive index materials.
  • a solution of 22.5 g of the polymer of Example I and 1.13 g of dicumyl peroxide in 77.5 g of cyclohexyl acetate was filtered through a 0.2 ⁇ m filter.
  • the solution was spin-coated at 1000 rpm for 30 sec and then cured in a vacuum oven which was heated from 20°C to 200°C in 1.5 h and then kept at 200°C for 30 min.
  • the resulting product was cooled slowly to give a cladding layer having a refractive index of 1.4676 and an optical loss of 0.15 dB/cm which was used in a penta-layered thermo-optical device according to PCT application WO 97/01782.
  • a reactor was charged with 122 g of hexafluoroisopropylidenedicyclo- hexanol, 100 g of triphosgene (bis(trichloromethyl) carbonate), and 1 I of dry toluene, under a nitrogen atmosphere.
  • the temperature of the reactants was lowered to approx. -3°C with stirring, after which 86.3 g of N,N-dimethylaniline diluted in 100 ml of dry toluene were added dropwise in 80 min.
  • reaction mixture was diluted with 200 ml of dry toluene, the temperature was raised to ca. 70°C, and the mixture was stirred for approx.

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  • Optical Integrated Circuits (AREA)

Abstract

The invention pertains to a cross-linkable fluorinated polymer comprising the carbonate moiety having formula (I) wherein n=1-10 and m=0-9. Preferably, the polymer further comprises a cross-linkable moiety derived from a diol selected from (II) and (III) wherein A, A1, and A2 are independently a bond or C1-12 alkylene, or together with the carbon atoms to which they are bonded form a 5- or 6-membered ring; B is independently O or C1-4 alkyl; Q is -CO-C(=E)D, wherein D is H or C1-4 alkyl; and E is C1-6 alkylidene;and each of the alkyl, alkylene, and alkylidene groups may be halogenated. The polymers of the invention can be used in cladding layers or waveguides, in particular for thermo-optical devices.

Description

POLYMERS COMPRISING A FLUORINATED CARBONATE MOIETY
The present invention is in the field of optical components, more particularly, polymeric optical components. By optical components are meant here, thermo-optical components, electro-optical components or passive components.
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.
Polymeric thermo-optical components generally comprise a polymeric three-layer structure on a substrate. The three-layer structure comprises a low refractive index lower cladding layer, a high refractive index core layer, and a low refractive index upper cladding layer. On top of the upper cladding layer heating elements are provided (usually metal strips) to heat the polymeric cladding and core material, 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. Polymeric electro-optical components in general also comprise a polymeric three-layer structure. The three-layer structure comprises a low refractive index lower cladding layer, a non-linear optically active, high refractive index core layer, and a low refractive index upper cladding layer. 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.
Optical components having an at least penta-layered polymer structure on a substrate comprising: a) a low refractive index lower 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 upper cladding layer, are also known in the art.
With this specific layer structure optimum transversal confinement can be obtained, which results in less loss of light and an improved switching efficiency.
For optical components preferably silicon substrates are used. These substrates are readily available on the market and are of homogeneous thickness. Furthermore, they are frequently used in integrated circuit techniques and apparatus. One disadvantage of silicon is its high refractive index. Due to this high refractive index the light of the propagating mode might leak into the silicon substrate. The low refractive index lower cladding layer a) is applied to prevent leaking of light from the propagating mode into the silicon substrate. When other substrates are used, the low refractive index lower cladding a) is also of advantage in controlling the confinement of the propagating mode. Using a low refractive index lower cladding a) of appropriate index and thickness gives ample freedom in designing the core-matching refractive index cladding layers b) and d) and the core layer c).
As described above, the optical components usually comprise metal electrodes on top of the upper cladding layer, either for use as heating elements or for applying an electric field. These electrodes are usually made of gold and/or other metals such as chromium, nickel, copper, platinum, or combinations or alloys thereof.
The low refractive index upper cladding e) is applied to prevent leaking of the light from the propagating mode into the attenuating (gold) electrodes. The refractive indices of the low refractive index lower and upper cladding layers a) and e) are usually (approximately) the same. Employing a low refractive index upper cladding layer e) with a larger thickness than that of the low refractive index lower cladding layer a) makes it possible to use a core-matching refractive index upper cladding layer d) which is thinner than the core-matching refractive index lower cladding b). In this case the resulting combined thickness of the low refractive index upper cladding d) and the core-matching refractive index upper cladding e) is smaller than the combined thickness of the low refractive index lower cladding a) and the core-matching refractive index lower cladding b). As a consequence, the structure is transversally asymmetric, with the core layer being close to the electrodes and thus experiencing stronger induced thermo-optical or electro-optical effects, resulting in a more efficient component.
The core-matching refractive index lower cladding b) and the core- matching refractive index upper cladding d) are applied to obtain transversal confinement of the propagating mode. The refractive index can be chosen in a relatively wide range to achieve the required properties, such as: monomode behavior, good overlap with a Standard Single Mode Fiber (SMF).
Lateral confinement can be achieved by all known methods for defining channels in planar waveguiding components. Suitable methods are:
1. shaping the core layer by etching techniques (for instance reactive ion etching with oxygen plasma) to obtain a buried channel waveguide,
2. bleaching the core layer to obtain a buried channel waveguide, 3. shaping either of the core-matching refractive index upper and lower cladding layers b) and d) to obtain a ridge (strip loaded) or an inverted ridge waveguide,
4. bleaching either of the core-matching refractive index upper and lower cladding layers b) and d) to obtain a ridge (strip loaded) or an inverted ridge waveguide. All these techniques are known to the artisan and need no further elucidation here. When using technique 1 , the core layer is etched away, leaving only the channel waveguide. Subsequently, core-matching refractive index upper cladding material is applied both on top of the core layer c) and onto the areas where the core material was etched away. This technique and also technique 2 are preferred because they can result in symmetrical channel waveguides. Symmetrical channel waveguides show low polarization dependence of the modal properties. When the bleaching technique is used, the refractive index of the core-matching refractive index cladding layers b) and d) should be adapted to the refractive index of the bleached parts of the core. When the shaping of the core technique is used, the refractive index of the core-matching refractive index upper cladding layer material is chosen such as to give the required properties, such as: monomode behavior, good overlap with a Standard Single Mode Fiber (SMF), low polarization dependence, low bend losses.
The polymers used for thermo-optical devices according to the invention are so-called optical polymers. Many optical polymers are known in the art, but there is still need for improvement. A particular problem of polymeric waveguides is the difference between the refractive indices of the core layer and the surrounding cladding layers. Typically, these index differences are in the range of 0.003 to 0.008. In waveguide switches switching is induced by index differences of 0.001 (digital switches) to 0.0001 (interferometer switches). These small index differences can be induced by thermo- or electro-optical properties of polymeric materials. In a thermo-optical switch the core index is lowered by locally heating the layer stack by means of a heating element. The closer the heater is to the core, the more efficiently this index lowering can be performed by a lower switching power. To prevent unwanted light absorption by the heater elements, it is advantageous to apply a low-index cladding layer between the waveguide and the heating element. The lower the index of the cladding layer is, the thinner this cladding layer can be, while leakage to the heater is still prevented. To prevent excess loss in the cladding layer and leakage to the substrate, this material must have a low absorption at the operating wavelengths (1.3 and 1.5 μm). It is therefore an object of the invention to provide polymeric material with very low refractive index, and very low optical loss, preferably less than 0.15 dB/cm. However, the polymeric material must also display high Tg because of chemical and optical stability, and be cross-linkable to obtain cladding layers suitable for thermo-optical waveguides. Moreover, when polymeric material is used as a waveguide core, it is advantageous to use material with an index similar to that of the optical fiber attached to said waveguide, which effective index for standard single mode fiber is 1.467 at 1.3 μm and 1.468 at 1.5 μm. When doped silica is used as a core, the polymers of the invention can be used advantageously as cladding because their refractive indices can be lower than that of the glass core, which has the advantage that these hybrid waveguides can be rendered athermal.
It has now been found that a cross-linkable fluorinated polymer comprising the carbonate moiety having the formula:
wherein n = 1-10 and m = 0-9 meets these demands. Preferably n =1-3 and m = 0-3.
The various layers can be applied by spin-coating. In order to be able to spin-coat layer-on-layer, it is often necessary to cross-link one layer before applying the next. Therefore, the optical polymers or NLO polymers are rendered cross-linkable either by the incorporation of cross-linkable monomers or by mixing cross-linkers such as polyisocyanates, polyepoxides, etc. into the polymer.
Preferably, the polymer further comprises a cross-linkable moiety derived from a diol selected from:
wherein
A, A^ and A2 are independently a bond or C1-12 alkylene, or together with the carbon atoms to which they are bonded form a 5- or 6-membered ring;
B is independently O or C1-4 alkyl;
Q is -CO-C(=E)D, wherein
D is H or C^ alkyl; and
E is C1-6 alkylidene; and each of the alkyl, alkylene, and alkylidene groups may be halogenated.
More preferably, the cross-linkable moiety is derived from the diol with the formula HO-CH2-CH(OH)-CH2-0-CO-C(=CH2)CH3.
The term C^ alkyl means an alkyl group with 1 to 4 carbon atoms, such as methyl, ethyl, propyl, isopropyl, butyl, terf-butyl, and the like. Methyl is the preferred alkyl group.
The term C1-12 alkylene means an alkylene group with 1 to 12 carbon atoms, such as methylene, ethylene, propylene, 2,2,-dimethylpropylene, dodecylene, and the like. A, A-,, and A2 are preferably a bond or an alkylene group with 1-3 carbon atoms.
The term C^6 alkylidene means an alkylidene group with 1 to 6 carbon atoms, such as methylene, ethylidene, propylidene, 2-methylpropylidene, and the like. Methylene and ethylidene are the preferred alkylidene groups.
When the alkyl, alkylene, or alkylidene groups are halogenated, chlorine and fluorine are the preferred halogens. Fluorine is the most preferred halogen. The index of the polymer can be fine-tuned by selecting the number, the type, and the combination of halogens.
The polymer of the invention can be prepared by standard methods known in the art for the preparation of similar polymers. For instance, the bischloroformate of hexafluorobisphenol A or hexafluoroisopropylidene- dicyclohexanediol bischloroformate can be polymerized in suitable solvents with the hexafluoro-perhydro-bisphenol A, the synthesis of which has been disclosed in EP 0,279,462, optionally in the presence of suitable cross- linkable moieties, such as the above-mentioned diols.
Non-linear electric polarization may give rise to several optically non-linear phenomena, such as frequency doubling, Pockels effect, and Kerr effect. In order to render polymeric non-linear optical material active (obtain the desired NLO effect macroscopically), the groups present in the polymer, usually hyperpolarizable side-groups, first have to be aligned (poled). Such alignment is commonly effected by exposing the polymeric material to electric (DC) voltage, the so-called poling field, with such heating as will render the polymeric chains sufficiently mobile for orientation. In order to enhance the stability of the thermo-optical component, oxygen scavengers and radical scavengers and the like may be added to the optical polymers. The invention is further illustrated by the following examples. EXAMPLE I
Hexafluoro-perhydro-bisphenol A (150.0 g), hexafluorobisphenol A bischloroformate (398.7 g), and 2,3-dihydroxypropyl methacrylate (68.9 g) were dissolved in a mixture of anhydrous dichloromethane (1.5 I) and anhydrous tetrahydrofuran (1 I). After cooling to 0°C, anhydrous pyridine (133.4 g) was added dropwise. After the addition, the reaction mixture was allowed to warm to room temperature and stirred overnight. The pyridine hydrochloride was filtered off and the filtrate was precipitated in 50 I of methanol. The precipitate was filtered off and washed with methanol. The polymer was dried overnight in vacuo at 5 kPa at 50°C. Yield 460 g. Mw 26,000; Mn 13,000; Tg 119-126°C; TGA 190°C.
EXAMPLE II
The optical loss and the Tg of prior art polymers (A-C) with normal refractive indices were compared with the optical loss of the very low refractive index polymer of Example I:
The optical loss and the Tg of prior art polymers (D-E) with very low refractive indices were compared with the optical loss of the very low refractive index polymer of Example I:
N.D. = not determined
Key (monomer composition in mole%):
legenda: S =
9a
T =
u =
V =
HO-CH 2-(CF 2)4-CH2-OH
w =
9b legenda: X =
CIOCO
Y =
z =
It may be concluded that the polymer of the invention has a Tg and an optical loss which are comparable with those of higher refractive index materials, whereas the Tg of the polymer of the invention is substantially higher than the Tg of other very low refractive index materials. 10
Example III
A solution of 22.5 g of the polymer of Example I and 1.13 g of dicumyl peroxide in 77.5 g of cyclohexyl acetate was filtered through a 0.2 μm filter. The solution was spin-coated at 1000 rpm for 30 sec and then cured in a vacuum oven which was heated from 20°C to 200°C in 1.5 h and then kept at 200°C for 30 min. The resulting product was cooled slowly to give a cladding layer having a refractive index of 1.4676 and an optical loss of 0.15 dB/cm which was used in a penta-layered thermo-optical device according to PCT application WO 97/01782.
Example IV
A reactor was charged with 122 g of hexafluoroisopropylidenedicyclo- hexanol, 100 g of triphosgene (bis(trichloromethyl) carbonate), and 1 I of dry toluene, under a nitrogen atmosphere.
The temperature of the reactants was lowered to approx. -3°C with stirring, after which 86.3 g of N,N-dimethylaniline diluted in 100 ml of dry toluene were added dropwise in 80 min.
The reaction mixture was diluted with 200 ml of dry toluene, the temperature was raised to ca. 70°C, and the mixture was stirred for approx.
50 h more under a stream of nitrogen to remove the excess phosgene and other volatile products.
After working up (extraction with 10% hydrochloric acid, water, and brine, drying on sodium sulfate, evaporation of toluene in vacuo, recrystallization from toluene/n-hexane 1/1.35 v/v, 0.28 g/ml, and drying) pure hexafluoro- isopropylidenedicyclohexanediol bischloroformate was obtained in approx.
33% overall yield.
To a stirred solution of 11.45 g of hexafluoroisopropylidenedicyclohexane- diol bischloroformate, 4.17 g of hexafluoroisopropylidenedicyclohexanol, and 1.95 g of dihydroxy-isopropylmethacrylate dissolved in 70 ml of tetra- 11 hydrofuran/dichloromethane 2.4/1 v/v were added dropwise 3.83 g of pyridine in 10 ml of tetrahydrofuran/dichloromethane 2.4/1 v/v at 20°C in approx. 60 min.
The reaction mixture was stirred overnight, the precipitate (pyridine. HCI salt) was removed by filtration. The polymer was precipitated by vigorous stirring in 1 I of methanol, collected, and stirred with fresh methanol. The product was collected by filtration and left to dry in a vacuum oven at 65°C to yield 11.2 g (approx. 70%) of a polymer the recurring unit of which has the formula:
Mw = 13,460 ; Mn = 6,470; polydispersity 2.08.
Refractive index at 1550 nm 1.4428 and at 1300 nm 1.4443.

Claims

12Claims:
1. A cross-linkable fluorinated polymer comprising the carbonate moiety having the formula:
wherein n = 1-10 and m = 0-9.
2. The polymer of claim 1 wherein n = 1-3 and m = 0-3.
3. The polymer of claim 1 or 2 further comprising a cross-linkable moiety derived from a diol selected from:
wherein A, A-,, and A2 are independently a bond or C1- 2 alkylene, or together with the carbon atoms to which they are bonded form a 5- or 6- membered ring;
B is independently O or C -4 alkyl;
Q is -CO-C(=E)D, wherein
D is H or C.,.4 alkyl; and
E is C.,_6 alkylidene; and each of the alkyl, alkylene, and alkylidene groups may be halogenated. 13
4. The polymer of claim 3 wherein the cross-linkable moiety is derived from the diol with the formula HO-CH2-CH(OH)-CH2-0-CO-C(=CH2)CH3.
5. A film comprising the polymer of any one of claims 1-4.
6. A waveguide comprising the polymer of any one of claims 1-4.
7. A cladding layer comprising the polymer of any one of claims 1-4.
8. A thermo-optical device comprising the polymer of any one of claims 1-4.
9. The thermo-optical device of claim 8 having an at least penta-layered polymer structure on a substrate comprising: a) a low refractive index lower 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 upper cladding layer, wherein the low refractive index upper cladding layer and, optionally, the low refractive index lower cladding layer comprise the polymer of any one of claims 1-4.
EP98909428A 1997-02-24 1998-02-04 Polymers comprising a fluorinated carbonate moiety Withdrawn EP0963395A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
EP98909428A EP0963395A1 (en) 1997-02-24 1998-02-04 Polymers comprising a fluorinated carbonate moiety

Applications Claiming Priority (6)

Application Number Priority Date Filing Date Title
EP97200511 1997-02-24
EP97200511 1997-02-24
US4162297P 1997-03-27 1997-03-27
US41622P 1997-03-27
PCT/EP1998/000717 WO1998038237A1 (en) 1997-02-24 1998-02-04 Polymers comprising a fluorinated carbonate moiety
EP98909428A EP0963395A1 (en) 1997-02-24 1998-02-04 Polymers comprising a fluorinated carbonate moiety

Publications (1)

Publication Number Publication Date
EP0963395A1 true EP0963395A1 (en) 1999-12-15

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CA (1) CA2282622A1 (en)

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO9838237A1 *

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