WO2022222235A1 - 一种基于液晶的芯片化滤波器 - Google Patents

一种基于液晶的芯片化滤波器 Download PDF

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WO2022222235A1
WO2022222235A1 PCT/CN2021/098064 CN2021098064W WO2022222235A1 WO 2022222235 A1 WO2022222235 A1 WO 2022222235A1 CN 2021098064 W CN2021098064 W CN 2021098064W WO 2022222235 A1 WO2022222235 A1 WO 2022222235A1
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liquid crystal
chip
resonant
straight waveguide
double
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PCT/CN2021/098064
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English (en)
French (fr)
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吴佳辰
黄文彬
黄敏
刘晓同
徐忻怡
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苏州大学
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Publication of WO2022222235A1 publication Critical patent/WO2022222235A1/zh

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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 
    • G02F1/13—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 liquid crystals, e.g. single liquid crystal display cells
    • 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 
    • G02F1/13—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 liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333—Constructional arrangements; Manufacturing methods
    • 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 
    • G02F1/13—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 liquid crystals, e.g. single liquid crystal display cells
    • G02F1/137—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 liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
    • G02F1/139—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 liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent

Definitions

  • the present invention relates to a filter, in particular to a chip filter based on liquid crystal.
  • This narrow-band filter should have the advantages of low insertion loss, high sharpness, and wide free spectral range.
  • This kind of filter not only has a very wide application prospect in the field of optical communication such as DWDM system and all-optical switching system, but also has wide application potential in multi-spectral imaging, high-precision spectral analysis and various sensing systems.
  • Diffraction gratings are widely used as optical filters in optical channel performance monitoring modules. Several diffraction wavelengths require several detectors. However, For a system with a large number of channels, replacing the diffraction grating with a tunable optical filter can greatly reduce the number of detectors and thus reduce the volume of the optical channel performance monitoring module; in addition, the fixed filter has a "shielding" property for out-of-band interference. , the tunable optical filter can find out-of-band interference in the process of wavelength tuning, so as to make timely corrections.
  • the dielectric film TFF filter needs to use the cascade of multiple F-P cavities to improve the device isolation, which will affect the stability of the output optical power.
  • the fiber grating type filter when the fiber grating type filter is applied to multi-channel demultiplexing, a large amount of FBG is required for the cascade structure; the reflection part of the circulator is used to have excess loss.
  • the tunability of photonic crystal filters using external magnetic, electric, and thermal energies has a common limitation: as these energies increase, the transmission peak wavelength does not shift linearly, so the tuning is not well controllable In addition, the transmission peak is not narrow enough, the tuning range is not wide enough, the filter structure is more complicated, and the actual preparation is quite difficult.
  • micro-ring resonator filter is developing towards multi-ring cascade, and it is necessary to solve the problem of inter-ring resonance tuning and precise control of coupling coefficient.
  • Tunable photonic crystal filters using applied magnetic, electric, and thermal energies share a common limitation: as these energies increase, the transmission peak wavelength does not shift linearly, so the tuning is not well controllable, and the transmission peak is not enough Narrow, the tuning range is not wide enough, the filter structure is more complicated, and the actual preparation is quite difficult.
  • Tunable optical filters as the core optical devices are also widely used in filters, sensors and optical imaging systems. In addition to high performance, the size of tunable optical filters also needs to be miniaturized.
  • the micro-ring resonant filter has received more and more attention and research by technicians. plays an increasingly important role.
  • the present invention proposes a chip filter based on liquid crystal.
  • a liquid crystal-based chip filter includes:
  • the chip substrate layer, the chip substrate layer is a liquid crystal layer in which liquid crystal molecules are distributed;
  • the chip guide core layer is arranged on the surface of the chip substrate layer, and the chip guide core layer is a liquid crystal layer with liquid crystal molecules distributed.
  • the waveguide part is used to realize the input of white light or multi-spectral light source and the output of light of any wavelength;
  • the driving electrode is used to drive the arrangement change of the liquid crystal molecules in the chip substrate layer, the double-straight waveguide part and the resonant cavity part, and change the refractive index of the corresponding part.
  • the invention is a chip filter based on liquid crystal, which adopts the modulation of liquid crystal to realize the tunable filtering function, and the main working band can cover the near-ultraviolet to near-infrared band and the main communication band under low voltage driving, and the volume is small and easy to integrate.
  • the double-straight waveguide part has a symmetrical structure.
  • the resonant cavity part includes: at least two resonant microrings cascaded with each other.
  • the filtering effect is good.
  • the radius of the resonant microring is above 4um
  • the diameter of the double-straight waveguide part is more than 2um
  • the overall structure of the chip filter is above 20um.
  • the output wavelength covers light in the wavelength band of 380 nm to 780 nm, so that the output light in the visible light band can be tunable.
  • the resonant microring has a symmetrical structure.
  • the resonant cavity part includes:
  • the first resonating micro-ring is transmissively coupled to the input straight waveguide in the dual straight waveguide portion;
  • a second resonant micro-ring cascaded with the first resonating micro-ring and transmissively coupled to the output straight waveguide in the dual straight waveguide section.
  • the structure is simple and the filtering effect is good.
  • the radius of the first resonant microring is larger than the radius of the second resonant microring.
  • the filtering effect is good.
  • the refractive index range of the liquid crystal of the chip substrate layer and the chip guiding core layer is between 1.55 and 1.70.
  • the orientation of liquid crystal molecules in the entire chip is patterned by photo-alignment technology, and the birefringence property of liquid crystal and voltage driving are used to realize the change of the refractive index of the core layer of the chip and the substrate layer of the chip with the orientation of the liquid crystal molecules. While changing, the refractive index changes in the range of 1.55 to 1.7.
  • an angle between 0 and ⁇ exists between the liquid crystal molecules in the chip guide core layer and the liquid crystal molecules in the chip substrate layer, and the liquid crystal refractive index of the chip guide core layer is greater than that of the chip substrate layer.
  • the driving electrode includes: a plurality of driving units for respectively driving the change of the liquid crystal molecular arrangement in the chip substrate layer, the double-straight waveguide part, and the resonant cavity part.
  • the driving electrode adopts a plurality of independent control modules to ensure the accuracy of control and the stability of the control system.
  • FIG. 1 is a schematic structural diagram of a chip filter provided by an embodiment of the present invention.
  • FIG. 2 is a schematic diagram of a microring provided by an embodiment of the present invention.
  • FIG. 3 is a schematic diagram of a resonance mode provided by an embodiment of the present invention.
  • FIG. 4 is a second schematic structural diagram of a chip filter provided by an embodiment of the present invention.
  • Fig. 5 is the arrangement of liquid crystal molecules and the patterned electrodes of the first resonant microring part provided by the embodiment of the present invention.
  • FIG. 6 is the arrangement of liquid crystal molecules and the patterned electrodes of the first straight waveguide part provided by the embodiment of the present invention.
  • FIG. 7 is an experimental diagram of the wavelength of the output wave provided by the specific embodiment of the present invention.
  • FIG. 8 is an experimental diagram of the output wave wavelength provided by the second embodiment of the present invention.
  • 1-dual straight waveguide part 11-first straight waveguide part, 12-second straight waveguide part, 2-resonant cavity part, 21-first resonant microring, 22-second resonating microring, 3-driving electrode.
  • ordinal numbers “first”, “second”, etc. to describe common objects merely refers to different instances of similar objects, and is not intended to imply that objects so described must have temporal, spatial, ordinal aspects, or be in any order. other ways in the given order.
  • the chip filter includes:
  • the chip substrate layer, the chip substrate layer is a liquid crystal layer in which liquid crystal molecules are distributed;
  • the chip guide core layer is arranged on the surface of the chip substrate layer, and the chip guide core layer is a liquid crystal layer with liquid crystal molecules distributed. , the double-straight waveguide part 1 is used to realize the input of white light or multi-spectral light source and the output of light of any wavelength;
  • the driving electrode 3 is used to drive the arrangement change of the liquid crystal molecules in the chip substrate layer, the double-straight waveguide part 1 and the resonant cavity part 2 to change the refractive index of the corresponding part.
  • the double straight waveguide part 1 includes: a first straight waveguide part 11 arranged at the input end of the resonant cavity part 2 and a second straight waveguide part 12 arranged at the lower end of the resonant cavity part 2 .
  • liquid crystal is used as the light transmission and modulation medium, and the functions of the double-straight waveguide part 1 and the resonant cavity part 2 are realized by arranging the molecular orientation of the liquid crystal micro-domain, and the electro-optical modulation effect of the liquid crystal is used to make the refractive index of the waveguide medium adjustable. tunable, thus making the filter wavelength tunable
  • the input light source is: white light or multi-spectral light source, which includes the near-infrared band to the near-ultraviolet band.
  • the input light can be a mixed light source, but only light in a specific band can be coupled into the structure of the resonator part 2 .
  • the input light is coupled into the core layer composed of liquid crystal molecules by means of transmission coupling, and the transmission coupling coefficient can be controlled by controlling the distance between the double-straight waveguide part 1 and the cavity part 2 .
  • a detection element such as a spectrometer can be placed at the output end of the double-straight waveguide part 1, and the detectable range includes the near-infrared band to the near-ultraviolet band.
  • the invention is a chip filter based on liquid crystal, which adopts the modulation of liquid crystal to realize the tunable filtering function, and the main working band can cover the near-ultraviolet to near-infrared band and the main communication band under low voltage driving, and the volume is small and easy to integrate.
  • the remaining features and techniques are the same, and the difference is that the double-straight waveguide portion 1 has a symmetrical structure.
  • the remaining features and techniques are the same, except that the resonant cavity part 2 includes: at least two resonant microrings cascaded with each other.
  • the filtering effect is good.
  • the radius of the resonant microring is above 4um
  • the diameter of the double-straight waveguide part 1 is more than 2um
  • the overall structure of the chip filter is above 20um.
  • the output wavelength covers light in the wavelength band of 380 nm to 780 nm, so that the output light in the visible light band can be tunable.
  • the resonant frequency of the resonant microring is determined by the effective refractive index, radius, and resonant wavelength series of the resonant cavity, and the variation range of the effective refractive index is limited, the radius of the resonant cavity and the resonant wavelength series vary widely, so in order to realize the visible light
  • the output light of the wavelength band is tunable, the radius of the resonant microring needs to be more than 4um, the diameter of the double-straight waveguide part 1 needs to be more than 2um, the overall structure of the filter needs to be more than 20um, and the wavelength of the output end covers the 380nm to 780nm band.
  • the effective refractive index of the resonating micro-ring resonating cavity is adjusted by voltage driving, and the resonant wavelength series will change at this time to realize the modulation of the resonant wavelength.
  • the optical alignment technology accuracy of liquid crystal molecules can reach 0.1um, so the structural accuracy of the filter can also reach 0.1um.
  • the resonant microring has a symmetrical structure.
  • the remaining features and techniques are the same, except that the resonant cavity part 2 includes:
  • the first resonating micro-ring 21 is coupled to the input straight waveguide in the double straight waveguide part 1 through transmission;
  • the second resonant microring 22 is cascaded with the first resonating microring 21 and is transmissively coupled with the output straight waveguide in the dual straight waveguide section 1 .
  • the structure is simple and the filtering effect is good.
  • the radius of the first resonant microring 21 is larger than the radius of the second resonating microring 22 .
  • the filtering effect is good.
  • the planar structure of the resonant cavity part 2 includes, but is not limited to, the cascading manner in the above embodiment, and the cascading manner includes multiple integration manners such as series integration, parallel integration, multi-segment integration, and array integration.
  • Different cascading methods may have the advantages of expanding the free spectral range, reducing crosstalk, flat passband, high stability, and small dispersion, but there may also be losses caused by center wavelength mismatch, high processing accuracy requirements, and temperature polarization. cause problems such as reduced stability.
  • Different cascading methods have their own advantages and disadvantages.
  • the series integration method is adopted, which has excellent performance indicators in all aspects but is difficult to prepare. In different application scenarios, the same liquid crystal photo-alignment technology can be used to complete different methods. cascading method.
  • the microring structure of the double-straight waveguide is used to filter the incident light, so that the chip filter can output tunable light; the driving electrode 3 is used to modulate the waveguide medium, and then the effective refractive index of the resonant cavity part 2 is changed to realize the output of any wavelength. monochromatic light.
  • the double-straight waveguide part 1 is formed by arranging liquid crystal molecules whose alignment directions are at a certain angle to form a stepped waveguide structure.
  • the refractive index of the liquid crystal in the core layer of the chip is greater than that of the liquid crystal in the substrate layer, so as to realize the total reflection propagation of light in the waveguide medium. .
  • the resonant cavity part 2 is formed by arranging liquid crystal molecules whose arrangement directions are at a certain angle to form a stepped waveguide resonant cavity.
  • the light is coupled from the first straight waveguide part 11 at the input end of the resonant cavity part 2 into the resonant cavity of the first resonant microring 21, and oscillates and propagates in the resonating cavity, and the resonating cavity of the first resonating microring 21 and the second resonating microring 22 resonate
  • the cavity forms resonance such that the waves propagating in the resonant cavity of the first resonant microring 21 are coupled into the resonating cavity of the second resonating microring 22 and propagate in oscillation in the resonating cavity.
  • the wave in the resonant cavity of the second resonant microring 22 is finally coupled into the second straight waveguide part 12 at the lower end, and output from the lower end.
  • Free spectral range refers to the spectral range between two resonant wavelengths.
  • the definition of FSR is: in is the length of the resonant cavity, and ⁇ m is the resonant wavelength of the resonant cavity R is the radius of the resonator, m is the number of resonances, and neff is the effective refractive index of the resonator.
  • a resonant wave ⁇ 1 exists in the resonant cavity of the first resonant microring 21 , and after the resonant cavity of the first resonating microring 21 and the resonating cavity of the second resonating microring 22 form resonance, there is a resonance in the resonating cavity of the second resonating microring 22 wave ⁇ 2 , the condition for resonance is At this time, the resonant wave ⁇ 2 in the resonant cavity of the second resonant microring 22 is finally coupled into the second straight waveguide portion 12 at the lower end and output from the lower end.
  • R 1 and R 2 are determined, n 1 and n 2 change.
  • To output modulated ⁇ ' 1 and ⁇ ' 2 it is necessary to find matching m' 1 and m' 2 , which is the frequency selection process.
  • the remaining features and techniques are the same, except that the refractive index of the liquid crystal of the chip substrate layer and the chip guide core layer ranges from 1.55 to 1.70.
  • the orientation of liquid crystal molecules in the entire chip is patterned by photo-alignment technology, and the birefringence property of liquid crystal and voltage driving are used to realize the change of the refractive index of the core layer of the chip and the substrate layer of the chip with the orientation of the liquid crystal molecules. While changing, the refractive index changes in the range of 1.55 to 1.7.
  • liquid crystal molecules in the chip guide core layer and the liquid crystal molecules in the chip substrate layer have an angle between 0 and ⁇ and the liquid crystal refractive index of the core layer of the chip is greater than the refractive index of liquid crystal of the substrate layer of the chip.
  • the driving electrode 3 includes: a plurality of driving electrodes for driving the chip substrate layer, the double-straight waveguide part 1, the resonant cavity respectively The driving unit in which the arrangement of liquid crystal molecules in part 2 changes.
  • the driving electrode 3 adopts a plurality of independent control modules to ensure the accuracy of control and the stability of the control system.
  • the driving electrode 3 adopts a patterned electrode, and by modulating the liquid crystal molecules, the change of the refractive index of the waveguide medium is realized, and then the modulation of the output wavelength is realized.
  • the material of the driving electrode 3 may be, but not limited to, ITO glass.
  • the electrode patterning method can be performed by patterning and orienting the ITO glass, so that the electrode pattern corresponds to the liquid crystal arrangement pattern, and the electrode patterning and the liquid crystal patterning alignment can be realized by the area exposure method.
  • the driving electrode 3 can be modulated in a variety of ways, such as voltage modulation, temperature modulation, magnetic field modulation, optical field modulation, or multiple modulation modes coexisting.
  • One is the electric field driving of the electrodes, which uses the electro-optic effect of the liquid crystal to drive the liquid crystal molecules to rotate by applying a voltage.
  • the change of the alignment direction of the liquid crystal molecules in the resonant cavity part 2 of the chip guide core layer and the chip substrate layer will make the resonant cavity part 2.
  • the change of the effective refractive index changes the resonant wavelength, and the change of the alignment direction of the liquid crystal molecules in the dual-straight waveguide portion 1 of the core layer of the chip will cause the filter to be switched.
  • photosensitive materials such as azo materials
  • the driving unit for driving the first straight waveguide portion 11 can control whether the incident light can propagate in the first straight waveguide portion 11, the aperture angle of the incident light, and the transmission coupling coefficient with the resonant microring, and is used for driving the first straight waveguide portion 11.
  • the driving unit of the two-straight waveguide part 12 can control the intensity of the output light wave and the transmission coupling coefficient with the resonant microring, and the driving unit used to drive the resonating microrings of the resonating cavity part 2 can control the effective refraction of the resonating cavity of each microring
  • the rate of change makes the resonance condition of the resonant cavity change, and then changes the resonance wavelength and the filtering range.
  • the transmissive structural resonator is composed of two straight waveguides coupled with a micro-ring, and the coupled structural model is shown in Figure 2.
  • the transmissive resonator has two output ends, namely the through end and the drop end.
  • E 1 the input laser
  • E 2 the straight end of the resonator
  • E 4 the other part of the light energy coupled into the resonator
  • the resonant modes circulate in each resonator and can interact.
  • one cavity can be viewed as the spectral fidelity value of the resonant wavelength of the other cavity. Therefore, when the resonance conditions of two isolated cavities are satisfied, some resonance modes are enhanced while others are weakened, a phenomenon known as the Vernier effect.
  • the conditional formula for resonance is expressed as:
  • the electro-optical modulation driving of the double-ring structure liquid crystal is adopted to realize various functions of the microcavity filter.
  • the effective refractive index range of the liquid crystal of the chip guide core layer and the chip substrate layer can reach 1.55 to 1.70, and the variation of the effective refractive index can reach about 0.2.
  • the three-layer waveguide structures of the first resonant microring 2131 , the second resonating microring 2232 and the double-straight waveguide part 1 are all symmetrical structures, and the liquid crystals of each part are arranged vertically to achieve maximum modulation There are patterned electrodes at the bottom of the integrated chip to achieve voltage modulation of liquid crystal molecules.
  • the refractive index of the medium of the double-straight waveguide part 1 is 1.7, and the refractive index of the external medium is 1.55, forming a three-layer waveguide structure, which is incident from the incident end and propagates through total reflection.
  • the refractive index of the medium of the first straight waveguide portion 11 is n 2 , and the refractive index of the external medium thereof is n 1 ;
  • the refractive index of the external medium of the first resonant microring 21 is n 3
  • the internal refractive index of the medium is n' 3
  • the effective refractive index is n 4 ;
  • the refractive index of the external medium of the second resonant micro-ring 22 is n 5
  • the internal refractive index of the medium is n' 5
  • the effective refractive index is n 6 ;
  • the refractive index of the medium of the second straight waveguide portion 12 is n 8
  • the refractive index of the outer medium thereof is n 7 .
  • the resonance formula of the resonant cavity It can be obtained that the wavelength of the resonant wave coupled into the first resonant microring 21 is 502 nm and the modulus is 200.
  • the resonant wave propagates in the resonant cavity of the first resonant microring 21 , resonates with the second resonating microring 22 , and is coupled into the second resonating microring 22 .
  • Resonance relationship It can be obtained that the radius of the second resonant microring 22 is 5um, the effective refractive index of the initial refractive index is 1.600, and the distance between the second resonating microring 21 is 100 nm.
  • the resonance formula of the resonant cavity It can be obtained that the wavelength of the resonant wave coupled into the second resonant microring 22 is 502 nm, and the modulus is 100.
  • the distance between the second resonant microring 22 and the second straight waveguide portion 12 at the lower end is 100 nm, the resonant wave is coupled into the second straight waveguide portion 12 and is totally reflected and transmitted, and a 502 nm monochromatic wave is output from the second straight waveguide portion 12 , to realize the filtering function, as shown in Figure 7.
  • the liquid crystal can be electro-optically modulated by the patterned electrodes, the effective refractive index of the double-straight waveguide part 1 and the resonant cavity part 2 can be changed, and then the wavelength of the resonant wave can be significantly changed to realize the dynamic modulation function.
  • the effective refractive index of the first resonant microring 21 is changed to 1.700
  • the wavelength of the resonant wave is changed to 628 nm
  • the modulus is changed to 170
  • the effective refractive index of the second resonant microring 22 is changed to 1.700
  • the wavelength of the resonant resonant wave becomes 628nm
  • the modulus becomes 85
  • the wavelength of the monochromatic light at the output also becomes 628nm, which completes the frequency conversion function of the filter, as shown in Figure 8.
  • the refractive indices of the first resonant micro-ring 21 and the second resonating micro-ring 22 may also be different according to the difference of the applied voltages, so as to realize modulation of other wavelengths.
  • the invention is a tunable filter based on liquid crystal.
  • the spectrum of the filter includes near-infrared band to near-ultraviolet band, but the output light is monochromatic light, the spectral half-width is 500GHz, and the output light wavelength range is 380nm to 780nm.
  • the invention can realize the laser tunable broadband wavelength dynamic modulation output function, the main working band can cover the near-ultraviolet to near-infrared band and the optical communication band under low voltage driving, and the volume is small and easy to integrate.
  • the present invention has the following differences.
  • the KDP crystal adopts electro-optic modulation, which is not as diverse as the liquid crystal material, and can realize various modulation methods such as electric field, light field, magnetic field, temperature, etc.
  • electro-optic modulation which is not as diverse as the liquid crystal material, and can realize various modulation methods such as electric field, light field, magnetic field, temperature, etc.
  • KDP crystals are larger in size, while the liquid crystal disclosed in the present invention has a planar structure, which is easier to integrate.
  • the refractive index of the SOI structure cannot be tuned, and can only be used for filtering and trapping of specific wavelengths; the structure is large and the manufacturing process is complex, requiring the use of ultraviolet lithography technology.
  • the microring is fabricated, the quality of the resonant cavity will be degraded due to defects in the photolithography process.
  • the present invention has simple structure and simple process.
  • the present invention discloses a chip filter based on liquid crystal, which has the following beneficial effects:
  • the present invention belongs to a chip-based integrated filter, which has a simple structure, a high degree of integration, and a small volume, and can realize multi-level cascade.
  • the arrangement change of the liquid crystal can realize the functions of waveguide and microcavity filtering, which can be realized by the integration of photo-alignment technology, and can be driven at a lower voltage.
  • the free spectral range is large, which can meet the use requirements of various bands, and achieve full coverage of ultraviolet to near-infrared bands and communication bands.
  • the filtered light is monochromatic light
  • the spectral half-width is 500GHz
  • the spectral modulation range is 380nm. to 780nm.

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  • Chemical & Material Sciences (AREA)
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Abstract

一种基于液晶的芯片化滤波器，包括：芯片衬底层，芯片衬底层为分布有液晶分子的液晶层；芯片导芯层，设置于芯片衬底层表面，芯片导芯层为分布有液晶分子的液晶层，芯片导芯层包括：双直波导部分（1）以及与双直波导部分（1）透射耦合的谐振腔部分（2），双直波导部分用于实现白光或者多光谱光源的输入以及任意波长光的输出；驱动电极（3），用于驱动芯片衬底层、双直波导部分（1）、谐振腔部分（2）内液晶分子的排布变化，改变其对应部分的折射率。采用液晶的调制实现可调谐的滤波功能，低电压驱动下主要工作波段可以覆盖近紫外至近红外波段和主要通讯波段，且体积小、易于集成。

Description

一种基于液晶的芯片化滤波器 技术领域
本发明涉及一种滤波器，具体涉及一种基于液晶的芯片化滤波器。
背景技术
基于近年来的技术需要，迫切需要一类性能优异的窄带滤波器。这种窄带滤波器应该具有:插入损耗小、锐度高、自由光谱范围宽等优点。这种滤波器不仅在DWDM系统、全光交换系统等光通信领域中具有极为广泛的应用前景，而且在多光谱成像、高精度光谱分析以及各类传感系统中，也具有广泛应用的潜力。
由于可调谐光滤波器的带宽及高成本等局限使得其没有被大规模投入使用，光通道性能监测模块中广泛采用衍射光栅作为光滤波器，有几个衍射波长就需要几个探测器，然而对于通道数目较多的系统，用可调谐光滤波器代替衍射光栅可以大大减小探测器的数目从而减小光通道性能监测模块的体积；另外，固定滤波器对带外干扰具有“遮蔽”性，可调谐光滤波器在波长调谐过程中可以发现带外干扰，以便做出及时修正。
高性能的可调谐光滤波器是近年来的关注话题，已有介质膜,F-P腔、微环谐振腔、光子晶体、光纤光栅等技术，但这些可调谐方式在技术上各自还存在一些问题：
现有的可见光滤波器存在以下问题：
对于F-P腔滤波器，各类F-P腔可调谐光滤波器精细度和自由光谱区难以同时满足光通道性能监测模块对选频和调谐范围的要求。
对于介质膜TFF滤波器，介质膜TFF滤波器需要利用多个F-P腔的级联提高器件隔离度，会影响输出光功率的稳定性。
对于光纤光栅型滤波器，光纤光栅型滤波器应用于多通道分波时，采用级联结构需大量的FBG；采用加环形器反射部分会有多余损耗。
对于光子晶体滤波器，光子晶体滤波器利用外加磁场、电场和热能实现可调有着共同的局限性:随着这些能量的增加，透射峰波长不是线性的移动，这样调谐不具有很好的可控性，且透射峰不够窄，调谐范围也不够宽，滤波器结构更加的复杂，实际制备相当困难。
微环谐振腔滤波器的研究在向多环级联发展，需解决环间谐振调谐与藕合系数精确控制问题。光子晶体滤波器利用外加磁场、电场和热能实现可调有着共同的局限性:随着这些能量的增加，透射峰波长不是线性的移动，这样调谐不具有很好的可控性，且透射峰不够窄，调谐范围也不够宽，滤波器结构更加的复杂，实际制备相当困难。可调谐光滤波器作为核心的光学器件还被广泛应用在滤波器、传感器和光成像系统中，除了高性能，可调谐光滤波器的尺寸也需要不断微小化。在其中各种方案中，微环谐振滤波器越来越受到技术人员的广泛关注和研究，在感检测、快慢光、码型转换、波长转换、光纤承载无线电波、滤波器、滤波器等领域中具有越来越重要的作用。
发明内容
为了解决上述技术问题，本发明提出了一种基于液晶的芯片化滤波器。
为了达到上述目的，本发明的技术方案如下：
一种基于液晶的芯片化滤波器包括：
芯片衬底层，芯片衬底层为分布有液晶分子的液晶层；
芯片导芯层，设置于芯片衬底层表面，芯片导芯层为分布有液晶分子的液晶层，芯片导芯层包括：双直波导部分以及与双直波导部分透射耦合的谐振腔部分，双直波导部分用于实现白光或者多光谱光源 的输入以及任意波长光的输出；
驱动电极，用于驱动芯片衬底层、双直波导部分、谐振腔部分内液晶分子的排布变化，改变其对应部分的折射率。
本发明一种基于液晶的芯片化滤波器，采用液晶的调制实现可调谐的滤波功能，低电压驱动下主要工作波段可以覆盖近紫外至近红外波段和主要通讯波段，且体积小、易于集成。
在上述技术方案的基础上，还可做如下改进：
作为优选的方案，双直波导部分为对称结构。
采用上述优选的方案，易于制备。
作为优选的方案，谐振腔部分包括：至少两个互相级联的谐振微环。
采用上述优选的方案，滤波效果佳。
作为优选的方案，谐振微环的半径在4um以上；
双直波导部分的直径在2um以上；
芯片化滤波器的整体结构在20um以上。
采用上述优选的方案，输出波长涵盖380nm至780nm波段的光，实现可见光波段的输出光可调谐。
作为优选的方案，谐振微环为对称结构。
采用上述优选的方案，易于制备。
作为优选的方案，谐振腔部分包括：
第一谐振微环，第一谐振微环与双直波导部分中的输入直波导透射耦合；
第二谐振微环，第二谐振微环与第一谐振微环级联，且与双直波导部分中的输出直波导透射耦合。
采用上述优选的方案，结构简单，且滤波效果好。
作为优选的方案，第一谐振微环的半径大于第二谐振微环的半径。
采用上述优选的方，滤波效果好.
作为优选的方案，芯片衬底层和芯片导芯层液晶折射率范围在1.55～1.70之间。
采用上述优选的方案，液晶分子在整个芯片的取向由光取向技术形成图案化排列，利用液晶的双折射性质和电压驱动实现芯片导芯层和芯片衬底层折射率随液晶分子的取向方式的变化而变化，折射率变化区间为1.55至1.7。
作为优选的方案，芯片导芯层内液晶分子与芯片衬底层内液晶分子之间存在角度在0至π之间的夹角，且芯片导芯层的液晶折射率大于芯片衬底层的液晶折射率。
采用上述优选的方案，实现光在波导介质中的全反射传播。
作为优选的方案，驱动电极包括：多个用于分别驱动芯片衬底层、双直波导部分、谐振腔部分内的液晶分子排布变化的驱动单元。
采用上述优选的方案，驱动电极采用多个独立的控制模组，保证控制的精确性和控制系统的稳定。
附图说明
为了更清楚地说明本发明实施例的技术方案，下面将对实施例中所需要使用的附图作简单地介绍，应当理解，以下附图仅示出了本发明的某些实施例，因此不应被看作是对范围的限定，对于本领域普通技术人员来讲，在不付出创造性劳动的前提下，还可以根据这些附图获得其他相关的附图。
图1为本发明实施例提供的芯片化滤波器的结构示意图之一。
图2为本发明实施例提供的微环原理图。
图3为本发明实施例提供的共振模式原理图。
图4为本发明实施例提供的芯片化滤波器的结构示意图之二。
图5为本发明实施例提供的第一谐振微环部分的液晶分子排布及 图案化电极。
图6为本发明实施例提供的第一直波导部分的液晶分子排布及图案化电极。
图7为本发明具体实施例一提供的输出波波长的实验图。
图8为本发明具体实施例二提供的输出波波长的实验图。
其中：1-双直波导部分，11-第一直波导部分，12-第二直波导部分，2-谐振腔部分，21-第一谐振微环，22-第二谐振微环，3-驱动电极。
具体实施方式
下面结合附图详细说明本发明的优选实施方式。
下面将结合本发明实施例中的附图，对本发明实施例中的技术方案进行清楚、完整地描述，显然，所描述的实施例仅仅是本发明一部分实施例，而不是全部的实施例。基于本发明中的实施例，本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例，都属于本发明保护的范围。
使用序数词“第一”、“第二”等等来描述普通对象仅仅表示涉及类似对象的不同实例，并且并不意图暗示这样被描述的对象必须具有时间上、空间上、排序方面或者以任意其它方式的给定顺序。
另外，“包括”元件的表述是“开放式”表述，该“开放式”表述仅仅是指存在对应的部件，不应当解释为排除附加的部件。
为了达到本发明的目的，一种基于液晶的芯片化滤波器的其中一些实施例中，如图1所示，该芯片化滤波器包括：
芯片衬底层，芯片衬底层为分布有液晶分子的液晶层；
芯片导芯层，设置于芯片衬底层表面，芯片导芯层为分布有液晶分子的液晶层，芯片导芯层包括：双直波导部分1以及与双直波导部分1透射耦合的谐振腔部分2，双直波导部分1用于实现白光或者多光谱光源的输入以及任意波长光的输出；
驱动电极3，用于驱动芯片衬底层、双直波导部分1、谐振腔部分2内液晶分子的排布变化，改变其对应部分的折射率。
其中，双直波导部分1包括：设置于谐振腔部分2输入端的第一直波导部分11和设置于谐振腔部分2下路端的第二直波导部分12。
在光子芯片中使用液晶作为光传输和调制介质，通过排布液晶微区分子指向，实现双直波导部分1和谐振腔部分2的功能，并利用液晶的电光调制效应，使得波导介质折射率可调，进而使得滤波器实现波长可调谐
输入光光源为：白光或者多光谱光源，其包含近红外波段至近紫外波段，输入光可以为混合光源，但只有特定波段的光才能耦合进入谐振腔部分2的结构中。输入光采用透射耦合的方式耦合进入液晶分子构成的导芯层，可以通过控制双直波导部分1和谐振腔部分2之间的距离控制透射耦合系数。
双直波导部分1的输出端可放置如光谱仪的探测元件，可探测范围包含近红外波段至近紫外波段。
本发明一种基于液晶的芯片化滤波器，采用液晶的调制实现可调谐的滤波功能，低电压驱动下主要工作波段可以覆盖近紫外至近红外波段和主要通讯波段，且体积小、易于集成。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，双直波导部分1为对称结构。
采用上述优选的方案，易于制备。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，谐振腔部分2包括：至少两个互相级联的谐振微环。
采用上述优选的方案，滤波效果佳。
进一步，谐振微环的半径在4um以上；
双直波导部分1的直径在2um以上；
芯片化滤波器的整体结构在20um以上。
采用上述优选的方案，输出波长涵盖380nm至780nm波段的光，实现可见光波段的输出光可调谐。
由于谐振微环的谐振频率由谐振腔的有效折射率、半径、谐振波长级数决定，而有效折射率的变化范围有限、谐振腔的半径和谐振波长级数变化范围较大，所以为了实现可见光波段的输出光可调谐，谐振微环的半径需要达到4um以上，双直波导部分1的直径需要达到2um以上，滤波器的整体结构需要达到20um以上，输出端波长涵盖380nm至780nm波段。
而当谐振微环谐振腔的半径确定后，电压驱动调节谐振微环谐振腔的有效折射率，此时谐振波长级数会发生变化，实现谐振波长的调制。液晶分子的光取向技术精度可以到0.1um，所以滤波器的结构精度也可以达到0.1um。谐振微环和直波导之间的间距越小、不同谐振微环之间的间距越小，则透射耦合系数越大，所以谐振微环和直波导之间的间距、不同谐振微环之间的间距可达0.1um以上。
进一步，谐振微环为对称结构。
采用上述优选的方案，易于制备。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，谐振腔部分2包括：
第一谐振微环21，第一谐振微环21与双直波导部分1中的输入直波导透射耦合；
第二谐振微环22，第二谐振微环22与第一谐振微环21级联，且与双直波导部分1中的输出直波导透射耦合。
采用上述优选的方案，结构简单，且滤波效果好。
进一步，第一谐振微环21的半径大于第二谐振微环22的半径。
采用上述优选的方，滤波效果好。
谐振腔部分2的平面结构包括且不限于上述实施例中的级联方式，级联方式包含串联集成、并联集成、多段集成、阵列集成等多种集成方式。不同的级联方式可能会有扩大自由光谱范围、减少串扰、通带平坦、稳定性高、色散小等优点，但也可能会有中心波长失配造成的损耗、加工精度要求高、温度极化造成稳定性降低等问题。不同的级联方式都包含各自的优缺点，该实施例中采用了串联集成的方式，各方面性能指标优异但制备难度较大，而在不同应用场景中可以通过同样的液晶光取向技术完成不同的级联方式。
使用双直波导的微环结构对入射光进行滤波，使得该芯片化滤波器输出可调谐光；使用驱动电极3对波导介质进行调制，进而改变谐振腔部分2的有效折射率，实现输出任意波长的单色光。
双直波导部分1采用排列方向成一定夹角的液晶分子排列而成，形成阶梯式波导结构，芯片导芯层液晶折射率大于衬底层液晶折射率，从而实现光在波导介质中的全反射传播。
谐振腔部分2采用排列方向成一定夹角的液晶分子排列而成，形成阶梯式波导谐振腔。
光从谐振腔部分2输入端的第一直波导部分11耦合进入第一谐振微环21谐振腔，并在该谐振腔中振荡传播，第一谐振微环21谐振腔和第二谐振微环22谐振腔形成共振，使得第一谐振微环21谐振腔中传播的波耦合进入第二谐振微环22谐振腔，并在该谐振腔中振荡传播。第二谐振微环22谐振腔中的波最后耦合进入下路端的第二直波导部分12中，从下路端输出，通过结构设计和参数匹配，实现设定波长的单色光输出。
自由光谱范围(FSR)，是指两个谐振波长之间的光谱范围。FSR的定义是：
Figure PCTCN2021098064-appb-000001
其中
Figure PCTCN2021098064-appb-000002
为谐振腔长，λ m为谐振腔的谐振波长
Figure PCTCN2021098064-appb-000003
R为谐振腔半径，m为谐振次数，n eff为谐 振腔的有效折射率。
两个半径不同微环滤波器的总FSR可以表示为：m 1FSR 1＝m 2FSR 2＝FSR total。在第一谐振微环21谐振腔中存在谐振波λ 1，在第一谐振微环21谐振腔和第二谐振微环22谐振腔形成共振后，在第二谐振微环22谐振腔中存在谐振波λ 2，共振的条件为
Figure PCTCN2021098064-appb-000004
此时第二谐振微环22谐振腔中的谐振波λ 2最后耦合进入下路端的第二直波导部分12中，从下路端输出。当R 1、R 2确定时，n 1、n 2发生变化，要想输出调制后的λ' 1、λ' 2，则需要找到匹配的m' 1、m' 2，即为选频过程。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，芯片衬底层和芯片导芯层液晶折射率范围在1.55～1.70之间。
采用上述优选的方案，液晶分子在整个芯片的取向由光取向技术形成图案化排列，利用液晶的双折射性质和电压驱动实现芯片导芯层和芯片衬底层折射率随液晶分子的取向方式的变化而变化，折射率变化区间为1.55至1.7。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，芯片导芯层内液晶分子与芯片衬底层内液晶分子之间存在角度在0至π之间的夹角，且芯片导芯层的液晶折射率大于芯片衬底层的液晶折射率。
采用上述优选的方案，实现光在波导介质中的全反射传播。
为了进一步地优化本发明的实施效果，在另外一些实施方式中，其余特征技术相同，不同之处在于，驱动电极3包括：多个用于分别驱动芯片衬底层、双直波导部分1、谐振腔部分2内的液晶分子排布变化的驱动单元。
采用上述优选的方案，驱动电极3采用多个独立的控制模组，保证控制的精确性和控制系统的稳定。
驱动电极3采用图案化电极，通过调制液晶分子，实现波导介质折射率的变化，进而实现输出波长的调制。进一步，驱动电极3材料可以但不限于为ITO玻璃。电极图案化方式可以通过对ITO玻璃进行图案化取向，使得电极图案和液晶排布图案相对应，电极图案化和液晶图案化对位可以通过区域曝光方式实现。
驱动电极3可采用多种方式进行调制，如电压调制、温度调制、磁场调制、光场调或多种调制方式并存等。
下面简单介绍两种驱动方式：
一种是电极的电场驱动，利用液晶的电光效应来通过施加电压来驱动液晶分子转动，芯片导芯层谐振腔部分2和芯片衬底层内的液晶分子排列方向发生变化会使得谐振腔部分2的有效折射率发生变化进而改变谐振波长，芯片导芯层双直波导部分1的液晶分子排列方向发生变化会使得滤波器存在开关。
一种是掺入光敏材料(例如偶氮材料)，在光场调制下，光敏材料会带来芯片导芯层和芯片衬底层液晶分子的转动，在光场驱动时还需要控制驱动光的聚焦、波长与光敏材料对应。
用于驱动第一直波导部分11的驱动单元可以控制入射光能否在第一直波导部分11中传播、入射光的孔径角以及和谐振微环之间的透射耦合系数，而用于驱动第二直波导部分12的驱动单元可以控制输出光波的强度以及和谐振微环之间的透射耦合系数，用于驱动谐振腔部分2各谐振微环的驱动单元可以控制各微环谐振腔的有效折射率，使得谐振腔的谐振条件发生改变，进而改变谐振波长以及滤波范围。
以上多种实施方式可交叉并行实现。
为了更好地理解上述内容，以下进行原理描述。
透射式结构谐振腔由两根直波导和微环耦合构成，耦合结构模型 如图2所示。透射式谐振腔有两个输出端，即直通端和下路端。设输入的激光为E 1，在耦合区域有一部分光能量通过直波导直接输出，即谐振腔的直通端，记为E 2；另一部分光能量耦合进入谐振腔记为E 4，这部分光在腔内绕环传输，每次经过耦合区域时，一部分光能量耦合到直波导，通过谐振腔的下行端口输出，记为E 5；而另一部分光则继续绕环传输，记为E 3，最终形成光的闭合回路。
在稳定状态下，通过两个耦合区域的光将达到一个动态均衡状态。用谐振腔的谐振公式表达即为：
Figure PCTCN2021098064-appb-000005
如图3所示，在耦合的回音廊模腔中，共振模式在各谐振器中循环，可以相互作用。在强相互作用的情况下，一个腔可以看作是另一个腔的共振波长的谱保真值。因此，当满足两个孤立腔的共振条件时，某些共振模式会增强，而其他模式会减弱，这种现象称为游标效应。用共振的条件公式表达即为：
Figure PCTCN2021098064-appb-000006
在其上实施例的基础上，举两个具体实施例。
实施例一：
采用双环结构液晶的电光调制驱动，实现微腔滤波器的各项功能，采用的级联方式如图4所示。芯片导芯层和芯片衬底层液晶的有效折射率范围可以达到1.55至1.70，有效折射率的变化可达0.2左右。
如图5和6所示，第一谐振微环2131、第二谐振微环2232和双直波导部分1的三层波导结构均为对称结构，各部分液晶排列方式均为垂直排列以实现最大调制量的目的，且集成芯片底部有图案化电极以实现电压调制液晶分子。
采用自然光入射，双直波导部分1介质折射率为1.7，外部介质折射率为1.55，构成三层波导结构，从入射端入射并全反射传播。
第一直波导部分11介质折射率为n 2，其外部介质折射率为n 1；
第一谐振微环21外部介质折射率为n 3，其内部质折射率为n' 3，有效折射率为n 4；
第二谐振微环22外部介质折射率为n 5，其内部质折射率为n' 5，有效折射率为n 6；
第二直波导部分12介质折射率为n 8，其外部介质折射率为n 7。
第一谐振微环21半径为10um，初始有效折射率为n 4＝1.600，和第一光直波导部分之间的间距为100nm。由谐振腔的谐振公式
Figure PCTCN2021098064-appb-000007
Figure PCTCN2021098064-appb-000008
可得，耦合进入第一谐振微环21的谐振波波长为502nm，模数为200。
谐振波在第一谐振微环21谐振腔中传播，和第二谐振微环22发生共振，耦合进入第二谐振微环22。由共振的关系式
Figure PCTCN2021098064-appb-000009
可得，第二谐振微环22半径为5um，初始折射率有效折射率为1.600，和第一谐振微环21之间的间距为100nm。
同样由谐振腔的谐振公式
Figure PCTCN2021098064-appb-000010
可得，耦合进入第二谐振微环22的谐振波波长为502nm，模数为100。
第二谐振微环22和下路端的第二直波导部分12的间距为100nm，谐振波耦合进入第二直波导部分12并进行全反射传输，从第二直波导部分12输出502nm的单色波，实现滤波功能，如图7所示。
由于液晶可由图案化电极进行电光调制，改变双直波导部分1和谐振腔部分2的有效折射率，进而可以显著改变谐振波的波长，实现动态调制功能。
在实施例二中，将第一谐振微环21的有效折射率改变为1.700，谐振波的波长变为628nm，模数变为170，而第二谐振微环22的有效折射率变为1.700，共振的谐振波波长变为628nm，模数变为85，输出端的单色光波长也变为628nm，完成了滤波器的变频功能，如图8 所示。第一谐振微环21和第二谐振微环22的折射率也可根据两者施加电压的不同而采用不同的折射率，进而实现其他波长的调制。
本发明一种基于液晶的可调谐滤波器，滤波器的光谱包含近红外波段至近紫外波段，但输出光为单色光，光谱半宽为500GHz，输出光波长范围为380nm至780nm。本发明可以实现激光可调谐的宽波段波长动态调制输出功能，低电压驱动下主要工作波段可以覆盖近紫外至近红外波段、光通信波段，且体积小、易于集成。
本发明与同类的微环滤波器相比，具有以下不同之处。
与基于KDP晶体的微环谐振腔的选频滤波器相比，KDP晶体采用电光调制，而不如液晶材料种类多样，可以实现电场、光场、磁场、温度等多种调制方式，进而可以使用在更加复杂的情况；KDP晶体体积较大，而本发明所公开的液晶为平面结构，更易集成。
与基于SOI的一阶或高阶环形滤波器相比，SOI结构的折射率无法调谐，只能用于特定波长的滤波和陷波；结构较大，制作工艺复杂，需要采用紫外光刻技术，而在制备微环时，会因为光刻工艺缺陷导致谐振腔的质量下降。而本发明结构简洁，工艺简单。
综上述，本发明公开一种基于液晶的芯片化滤波器，其具有以下有益效果：
第一，本发明属于芯片化集成滤波器，结构简洁，集成化程度高，体积小，可以实现多级级联。
第二，液晶的排布变化可以实现波导和微腔滤波的功能，可以利用光取向技术一体化实现，较低电压即可驱动。
第三，自由光谱范围大，可以满足多种波段的使用要求，实现紫外到近红外波段、通讯波段的全覆盖，滤波后的光为单色光，光谱半宽为500GHz，光谱调制范围为380nm至780nm。
上述实施例只为说明本发明的技术构思及特点，其目的在于让本领域普通技术人员能够了解本发明的内容并加以实施，并不能以此限 制本发明的保护范围，凡根据本发明精神实质所作的等效变化或修饰，都应涵盖在本发明的保护范围内。

Claims (10)

  1. 一种基于液晶的芯片化滤波器，其特征在于，包括：
    芯片衬底层，所述芯片衬底层为分布有液晶分子的液晶层；
    芯片导芯层，设置于所述芯片衬底层表面，所述芯片导芯层为分布有液晶分子的液晶层，所述芯片导芯层包括：双直波导部分以及与所述双直波导部分透射耦合的谐振腔部分，所述双直波导部分用于实现白光或者多光谱光源的输入以及任意波长光的输出；
    驱动电极，用于驱动所述芯片衬底层、双直波导部分、谐振腔部分内液晶分子的排布变化，改变其对应部分的折射率。
  2. 根据权利要求1所述的芯片化滤波器，其特征在于，所述双直波导部分为对称结构。
  3. 根据权利要求1所述的芯片化滤波器，其特征在于，所述谐振腔部分包括：至少两个互相级联的谐振微环。
  4. 根据权利要求3所述的芯片化滤波器，其特征在于，
    所述谐振微环的半径在4um以上；
    所述双直波导部分的直径在2um以上；
    所述芯片化滤波器的整体结构在20um以上。
  5. 根据权利要求3所述的芯片化滤波器，其特征在于，所述谐振微环为对称结构。
  6. 根据权利要求3所述的芯片化滤波器，其特征在于，所述谐振腔部分包括：
    第一谐振微环，所述第一谐振微环与所述双直波导部分中的输入直波导透射耦合；
    第二谐振微环，所述第二谐振微环与所述第一谐振微环级联，且与所述双直波导部分中的输出直波导透射耦合。
  7. 根据权利要求6所述的芯片化滤波器，其特征在于，所述第一谐振微环的半径大于所述第二谐振微环的半径。
  8. 根据权利要求1-7任一项所述的芯片化滤波器，其特征在于，所述芯片衬底层和芯片导芯层液晶折射率范围在1.55～1.70之间。
  9. 根据权利要求1-7任一项所述的芯片化滤波器，其特征在于，所述芯片导芯层内液晶分子与所述芯片衬底层内液晶分子之间存在角度在0至π之间的夹角，且所述芯片导芯层的液晶折射率大于所述芯片衬底层的液晶折射率。
  10. 根据权利要求1-7任一项所述的芯片化滤波器，其特征在于，所述驱动电极包括：多个用于分别驱动所述芯片衬底层、双直波导部分、谐振腔部分内的液晶分子排布变化的驱动单元。
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Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5361320A (en) * 1993-02-19 1994-11-01 University Of Colorado Foundation Liquid crystal fiber waveguide
KR20060121438A (ko) * 2005-05-24 2006-11-29 엘지전자 주식회사 마이크로 링 광 공진기 및 그 제조방법
CN1886686A (zh) * 2003-12-24 2006-12-27 皮雷利&C.有限公司 低损耗微环形谐振器设备
US20070258677A1 (en) * 2006-04-24 2007-11-08 The Hong Kong University Of Science And Technology Electrically Tunable Microresonators Using Photoaligned Liquid Crystals
CN101840029A (zh) * 2010-04-28 2010-09-22 中国科学院半导体研究所 一种集成化可重构光插分复用器
CN102841407A (zh) * 2012-09-20 2012-12-26 电子科技大学 一种波导型偏振光分束器
CN103760699A (zh) * 2014-02-19 2014-04-30 华中科技大学 基于液晶狭缝波导的微环谐振腔型可调谐光滤波器
CN107991738A (zh) * 2017-12-08 2018-05-04 华中科技大学 一种硅基多功能可重构光滤波器
CN214411755U (zh) * 2021-04-22 2021-10-15 苏州大学 一种基于液晶的可调谐激光器
CN214409494U (zh) * 2021-04-22 2021-10-15 苏州大学 一种基于液晶的芯片化滤波器

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5361320A (en) * 1993-02-19 1994-11-01 University Of Colorado Foundation Liquid crystal fiber waveguide
CN1886686A (zh) * 2003-12-24 2006-12-27 皮雷利&C.有限公司 低损耗微环形谐振器设备
KR20060121438A (ko) * 2005-05-24 2006-11-29 엘지전자 주식회사 마이크로 링 광 공진기 및 그 제조방법
US20070258677A1 (en) * 2006-04-24 2007-11-08 The Hong Kong University Of Science And Technology Electrically Tunable Microresonators Using Photoaligned Liquid Crystals
CN101840029A (zh) * 2010-04-28 2010-09-22 中国科学院半导体研究所 一种集成化可重构光插分复用器
CN102841407A (zh) * 2012-09-20 2012-12-26 电子科技大学 一种波导型偏振光分束器
CN103760699A (zh) * 2014-02-19 2014-04-30 华中科技大学 基于液晶狭缝波导的微环谐振腔型可调谐光滤波器
CN107991738A (zh) * 2017-12-08 2018-05-04 华中科技大学 一种硅基多功能可重构光滤波器
CN214411755U (zh) * 2021-04-22 2021-10-15 苏州大学 一种基于液晶的可调谐激光器
CN214409494U (zh) * 2021-04-22 2021-10-15 苏州大学 一种基于液晶的芯片化滤波器

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