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CN111812908B - Fabry-Perot Cavity Filter and Method for Dynamic Color Control - Google Patents

Fabry-Perot Cavity Filter and Method for Dynamic Color Control Download PDF

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CN111812908B
CN111812908B CN202010719177.2A CN202010719177A CN111812908B CN 111812908 B CN111812908 B CN 111812908B CN 202010719177 A CN202010719177 A CN 202010719177A CN 111812908 B CN111812908 B CN 111812908B
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metal
transparent conductive
fabry
conductive oxide
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CN111812908A (en
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蒋向东
李明成
许文瑞
王继岷
李伟
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University of Electronic Science and Technology of China
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/21Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  by interference
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/0009Materials therefor
    • G02F1/0063Optical properties, e.g. absorption, reflection or birefringence
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/0102Constructional details, not otherwise provided for in this subclass
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/0121Operation of devices; Circuit arrangements, not otherwise provided for in this subclass
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/23Devices 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  for the control of the colour

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)

Abstract

The invention provides a Fabry-Perot cavity filter for dynamic color regulation and control, a preparation method and a tuning method, which sequentially comprise a first metal film layer, a second non-conductive dielectric layer, a third transparent conductive oxide layer, a fourth metal layer and a fifth substrate layer from top to bottom; the second non-conductive dielectric layer is used as a barrier layer to block metal ion migration of a material with a dielectric constant of being close to 0 after electrochemical metallization; the third transparent conductive oxide layer is made of a material with a dielectric constant of 0, and the refractive index can be changed under the action of an electric field, so that the refractive index of the Fabry-Perot cavity body is adjusted; the invention realizes the change of the effective refractive index of the ENZ material based on the ECM effect, thereby changing the resonance wavelength of the FP cavity, effectively solving the problems and completing the memory of the resonance condition while removing the voltage.

Description

Fabry-Perot cavity filter and method for dynamic color regulation
Technical Field
The invention belongs to the technical field of display, and particularly relates to a Fabry-Perot cavity filter for dynamic color regulation and control, and a preparation method and a tuning method thereof.
Background
In the field of display technology, plasma structures can be used to generate different colors, but once the structures are determined, the generated colors are fixed. The plasma structure has the characteristics of thin structure, stability, high resolution and the like in the display technology. How to dynamically adjust the color of the plasma is a hotspot of current research, most of the ideas of dynamic adjustment are to change the structure of the plasma so as to adjust the intensity or wavelength of the plasma, and the current main regulation and control mode is mainly based on: direct electrochemical control, reversible electrochemical deposition, polarization control, a pullable embedded structure, a phase change material, and electromechanical control of the distance between two metals of a fabry-perot (FP) cavity. The invention mainly realizes the dynamic adjustment of colors based on the FP cavity.
FP cavities are typically a special optical structure formed by two high reflectivity metal layers and an intermediate layer cavity. Incident light beams can generate a multi-beam interference effect in the cavity, light waves meeting the phase matching condition can generate resonance, and the resonance wavelength is related to the cavity length and the cavity refractive index.
However, most FP cavities choose to adjust the resonant wavelength by adjusting the cavity length in two main ways: the first is to prepare FP cavities of different cavity lengths, but this does not allow for a truly dynamic adjustment, and the second is to electrostatically adjust the distance between the two metal plates, but such devices are expensive to manufacture and complex to manufacture, and the mechanical device lifetime decreases with time.
The FP cavity that changes the resonance wavelength by changing the cavity refractive index is reported, and the reason for this is because the refractive index of the material that can be used as the FP cavity is not easily changed. The material with the dielectric constant tending to 0 (Epsilon-near-zero) ENZ material refers to the material with the real part of the dielectric constant tending to 0 in a specific wavelength interval. Based on the change Δ n of the refractive index of the material ═ Δ ∈/2(2 √ ε), when ε tends to 0, a large change in refractive index can be obtained with a theoretically limited change in dielectric constant. The metal ions in the ENZ material under bias, due to the electrochemical metallization (ECM) occurring, also enable dynamic adjustment and memory of the refractive index. Therefore, based on the technology, the FP cavity based on the ENZ material is designed, and the function of dynamically regulating and controlling the color can be realized by changing the resonance wavelength.
Disclosure of Invention
Aiming at the problem that the length of the Fabry-Perot (FP) cavity is adjusted to adjust the resonance wavelength and the resonance intensity, the invention provides the FP cavity which uses a material (ENZ material) with a dielectric constant of being close to 0 as a cavity material, the resonance wavelength and the resonance intensity are adjusted by dynamically adjusting the refractive index of the ENZ material by applying voltage so as to achieve the purpose of adjusting color, and the memory of the color is completed after the voltage is removed.
In order to achieve the purpose, the technical scheme of the invention is as follows:
a Fabry-Perot cavity filter for dynamic color regulation comprises a first metal film layer 11, a second non-conductive dielectric layer 12, a third transparent conductive oxide layer 13, a fourth metal layer 14 and a fifth substrate layer 15 from top to bottom in sequence;
the first metal thin film layer 11 is used for introducing incident light into the fabry-perot cavity and is used as an upper metal layer in a metal-insulator-metal structure of the fabry-perot cavity;
the second non-conductive dielectric layer is used as an intermediate dielectric layer 12 in a metal-insulator-metal structure of a Fabry-Perot cavity and is used as a barrier layer for blocking metal ion migration after electrochemical metallization of a material (ENZ material) with a dielectric constant of being close to 0;
the third transparent conductive oxide layer 13 is made of a material with a dielectric constant of about 0, and can change the refractive index under the action of an electric field, so that the refractive index of the Fabry-Perot cavity is adjusted;
the fourth metal layer 14 is used as a lower metal layer in a fabry-perot cavity metal-insulator-metal structure;
the bottom is a fifth layer substrate layer 15 on which the above structure is prepared;
meanwhile, a first metal thin film layer 11, a second non-conductive dielectric layer 12, a third transparent conductive oxide layer 13 and a fourth metal layer 14 form a memristive unit, wherein the first metal thin film layer 11 serves as a first electrode, the fourth metal layer serves as a second electrode 14, the first metal thin film layer 11 and the second non-conductive dielectric layer 12 form a mutually perpendicular crossed array (CROSSBAR) structure, the second non-conductive dielectric layer 12 and the third transparent conductive oxide layer 13 form a mutually perpendicular crossed array structure, the first electrode is electrically connected with the second electrode, voltage is applied to the memristive unit to complete the regulation and control of the refractive index, the voltage is removed, and the refractive index completes the memory.
Preferably, the first metal thin film layer 11 is Au, the thickness of the Au film ensures that incident light can penetrate through the Au film and enter the FP cavity, and the thickness of the Au film is 15-30 nm.
Preferably, the second non-conductive dielectric layer 12 is a titanium dioxide layer, TiO2TiO as non-conductive dielectric to form an electric field in the memristive cell2The layer thickness is 50-100 nm.
Preferably, the third transparent conductive oxide layer 13 is a silica-doped silver thin film layer, SiO2The preset volume fraction of Ag is 90%: the silicon dioxide silver-doped thin film layer exists in the area of the real part of the dielectric constant area 0, and the thickness of the silicon dioxide silver-doped thin film layer is 75-150 nm.
Preferably, the fourth metal layer 14 is an Au layer, and the thickness of the Au layer is 200-300 nm.
Preferably, the fifth layer substrate layer 15 is a Si substrate layer, and the thickness thereof is 15 mm.
In order to achieve the above object, the present invention further provides a method for preparing a fabry-perot cavity filter for dynamic color control, comprising the following steps:
(1) depositing an Au film on the fifth substrate layer 15 by using a direct-current magnetron sputtering mode;
(2) depositing a silicon dioxide silver-doped transparent conductive film on the fourth metal layer 14 in a radio frequency magnetron co-sputtering mode, and patterning the layer of material by using a mask;
(3) depositing TiO2 on the third transparent conductive oxide layer 13 by using a direct-current magnetron sputtering mode, and patterning the layer of material by using a mask;
(4) depositing an Ag film on the second non-conductive dielectric layer 12 by using a direct current magnetron sputtering method, and patterning the layer of material by using a mask to form an electrode.
In order to achieve the above object, the present invention further provides a method for tuning the resonance wavelength and the resonance intensity of the fabry-perot cavity filter for dynamic color control, comprising the following steps:
filter pair x when no voltage is applied1The wavelength has strong absorption and presents a color, a positive voltage is applied to the fourth metal layer 14 through a voltage device, Ag atoms in the third transparent conductive oxide layer 13 can be subjected to electrochemical metallization, Ag is pre-embedded in the third transparent conductive oxide layer, adjacent Ag clusters are equivalent to two electrodes, Ag atoms can form Ag nanowires between the Ag clusters through oxidation-reduction reaction, the effective refractive index of the third transparent conductive oxide layer is changed, the Ag nanowires close to the interface of the second non-conductive dielectric layer and the third transparent conductive oxide layer can be blocked at the interface to form an Ag layer, and the refractive index of the third transparent conductive oxide layer is changed along with the formation of the Ag nanowires at the moment, so that the Ag layer can be subjected to x-ray color correction2The wavelength has strong absorption and shows b color; as the positive voltage is further applied to the fourth metal layer, Ag nano-wires in the third transparent conductive oxide layer are further formed, the refractive index is continuously changed, and the x is subjected to the positive voltage3The wavelength has strong absorption and shows c color;
applying positive voltage to the first metal film layer 11 by a voltage device, the Ag atoms continue to generate electrochemical metallization effect, the Ag nanowires of the third transparent conductive oxide layer start to break gradually, the refractive index changes, and the X pairs2The wavelength has strong absorption and shows b color, and as a positive voltage is further applied to the first metal thin film layer 11, Ag nano-wires formed in the third transparent conductive oxide layer are completely broken, the refractive index returns to the initial value, and the refractive index is adjusted to x1The wavelength has strong absorption and exhibits a color.
The invention has the beneficial effects that: most reports about the dynamic adjustment of the FP cavity currently adjust the resonance mode of the FP cavity by electromechanically controlling the thickness of the cavity between two metal plates, but this kind of FP cavity has mechanical loss, and the change of the cavity length inevitably causes the design problem of the device structure. The invention realizes the change of the effective refractive index of the ENZ material based on the ECM effect, thereby changing the resonance wavelength of the FP cavity, effectively solving the problems and completing the memory of the resonance condition while removing the voltage.
Drawings
FIG. 1 is a schematic perspective view of the present invention;
FIG. 2 is a top view of the structure provided by the present invention;
FIG. 3 is a schematic structural diagram of a voltage modulation unit according to the present invention;
FIG. 4 is a schematic diagram of a voltage modulation process according to the present invention;
FIG. 5 is a diagram of simulation results of the present invention.
1 is a Fabry-Perot cavity; 2 is an Ag accumulation layer, and 11 is a first metal film layer; 12 is a second non-conductive dielectric layer; 13 is a third transparent conductive oxide layer; 14 is a fourth metal layer; 15 is a fifth substrate layer;
Detailed Description
The embodiments of the present invention are described below with reference to specific embodiments, and other advantages and effects of the present invention will be easily understood by those skilled in the art from the disclosure of the present specification. The invention is capable of other and different embodiments and of being practiced or of being carried out in various ways, and its several details are capable of modification in various respects, all without departing from the spirit and scope of the present invention.
A Fabry-Perot cavity filter for dynamic color regulation comprises a first metal film layer 11, a second non-conductive dielectric layer 12, a third transparent conductive oxide layer 13, a fourth metal layer 14 and a fifth substrate layer 15 from top to bottom in sequence;
the first metal thin film layer 11 is used for introducing incident light into the fabry-perot cavity and is used as an upper metal layer in a metal-insulator-metal structure of the fabry-perot cavity;
the second non-conductive dielectric layer is used as an intermediate dielectric layer 12 in a metal-insulator-metal structure of a Fabry-Perot cavity and is used as a barrier layer for blocking metal ion migration after electrochemical metallization of a material with a dielectric constant of being close to 0;
the third transparent conductive oxide layer 13 is made of a material with a dielectric constant of about 0, and can change the refractive index under the action of an electric field, so that the refractive index of the Fabry-Perot cavity is adjusted;
the fourth metal layer 14 is used as a lower metal layer in a fabry-perot cavity metal-insulator-metal structure;
the bottom is a fifth layer substrate layer 15 on which the above structure is prepared;
meanwhile, a first metal thin film layer 11, a second non-conductive dielectric layer 12, a third transparent conductive oxide layer 13 and a fourth metal layer 14 form a memristive unit, wherein the first metal thin film layer 11 serves as a first electrode, the fourth metal layer serves as a second electrode 14, the first metal thin film layer 11 and the second non-conductive dielectric layer 12 form a mutually perpendicular crossed array (CROSSBAR) structure, the second non-conductive dielectric layer 12 and the third transparent conductive oxide layer 13 form a mutually perpendicular crossed array structure, the first electrode is electrically connected with the second electrode, voltage is applied to the memristive unit to complete the regulation and control of the refractive index, the voltage is removed, and the refractive index completes the memory.
The first metal film layer 11 is made of Au, the thickness of the Au film ensures that incident light can penetrate through the Au film to enter the FP cavity, and the thickness of the Au film is 15-30 nm.
The second non-conductive dielectric layer 12 is a titanium dioxide layer, TiO2TiO as non-conductive dielectric to form an electric field in the memristive cell2The layer thickness is 50-100 nm.
The third transparent conductive oxide layer 13 is a silicon dioxide silver-doped thin film layer, SiO2The preset volume fraction of Ag is 90%: the silicon dioxide silver-doped thin film layer exists in the area of the real part of the dielectric constant area 0, and the thickness of the silicon dioxide silver-doped thin film layer is 75-150 nm.
The fourth metal layer 14 is an Au layer with a thickness of 200-300 nm.
The fifth layer substrate layer 15 is a Si substrate layer and has a thickness of 15 mm.
The embodiment also provides a method for preparing the fabry-perot cavity filter for dynamic color control, which comprises the following steps:
(1) depositing an Au film on the fifth substrate layer 15 by using a direct-current magnetron sputtering mode;
(2) depositing a silicon dioxide silver-doped transparent conductive film on the fourth metal layer 14 in a radio frequency magnetron co-sputtering mode, and patterning the layer of material by using a mask;
(3) depositing TiO2 on the third transparent conductive oxide layer 13 by using a direct-current magnetron sputtering mode, and patterning the layer of material by using a mask;
(4) depositing an Ag film on the second non-conductive dielectric layer 12 by using a direct current magnetron sputtering method, and patterning the layer of material by using a mask to form an electrode.
The embodiment further provides a method for tuning the resonance wavelength and the resonance intensity of the fabry-perot cavity filter for dynamic color control, which includes the following steps:
filter pair x when no voltage is applied1The wavelength has strong absorption and presents a color, a positive voltage is applied to the fourth metal layer 14 through a voltage device, Ag atoms in the third transparent conductive oxide layer 13 can be subjected to electrochemical metallization, Ag is pre-embedded in the third transparent conductive oxide layer, adjacent Ag clusters are equivalent to two electrodes, Ag atoms can form Ag nanowires between the Ag clusters through oxidation-reduction reaction, the effective refractive index of the third transparent conductive oxide layer is changed, the Ag nanowires close to the interface of the second non-conductive dielectric layer and the third transparent conductive oxide layer can be blocked at the interface to form an Ag layer, and the refractive index of the third transparent conductive oxide layer is changed along with the formation of the Ag nanowires at the moment, so that the Ag layer can be subjected to x-ray color correction2The wavelength has strong absorption and shows b color; as the positive voltage is further applied to the fourth metal layer, Ag nano-wires in the third transparent conductive oxide layer are further formed, the refractive index is continuously changed, and the x is subjected to the positive voltage3The wavelength has strong absorption and shows c color;
applying positive voltage to the first metal film layer 11 by the voltage device, the Ag atoms continue to generate electrochemical metallization effectThe Ag nanowires of the third transparent conductive oxide layer begin to fracture gradually, and the refractive index changes for x2The wavelength has strong absorption and shows b color, and as a positive voltage is further applied to the first metal thin film layer 11, Ag nano-wires formed in the third transparent conductive oxide layer are completely broken, the refractive index returns to the initial value, and the refractive index is adjusted to x1The wavelength has strong absorption and exhibits a color.
Specifically, in this embodiment, as shown in fig. 1 and fig. 2, each device may be regarded as a plurality of FP cavity control units through the structural design of the cross array (cross array) perpendicular to each other, and different control units can achieve different adjustment effects, so as to achieve control over the entire adjustment effect, and meanwhile, the cross array (cross array) structure can ensure that the ohmic contact is sufficiently small.
As shown in fig. 3, the FP cavity control unit includes a first metal thin film layer 11, a second non-conductive dielectric layer 12, a third transparent conductive oxide layer 13, a fourth metal layer 14 and a fifth substrate layer 15. In the first metal thin film layer 11, the metal material is preferably Au, and in order to enable light to well penetrate through the first metal thin film layer 11, the thickness of Au should not be too thick, in this embodiment, a simulation study is performed by using 30nm Au. Said second non-conductive dielectric layer 13 is preferably TiO2,TiO2The titanium dioxide is used as a barrier layer in a memristor, can effectively block the migration of Ag ions, and adopts TiO with the thickness of 50nm2The film was subjected to simulation studies. The third transparent conductive oxide layer 13 is preferably SiO2The Ag-doped film can realize the migration of Ag atoms in the third transparent conductive oxide layer 13 through the ECM effect under the action of an electric field so as to achieve the purpose of adjusting the effective refractive index of the third transparent conductive oxide layer 12, and the SiO film2The Ag-doped thin film is also a typical transparent conductive thin film, and the proper doping amount enables the thin film to have an ENZ region in an optical band, so that the change of a dielectric constant is small, a large enough effective refractive index change can be provided, and a modulation effect is enhanced; in order to achieve the effects of transparency and conductivity, the invention adopts SiO with the thickness of 30nm2The initial doping amount of the Ag-doped film is Si02: ag (90%) was subjected to simulation study. The fourth metal layer 14 is preferably an Au layer, and in order to enable light to be effectively reflected back to the cavity, the simulation research is carried out by using Au with the thickness of 200 nm. The fifth layer substrate layer 15 is preferably a Si substrate with a thickness of 15 mm. The voltage regulating device is arranged on the first metal thin film layer 11 and the fourth metal thin film layer 14, an initial positive voltage is applied to the fourth metal thin film layer 14, and a negative voltage is applied to the first metal thin film layer 11.
As shown in fig. 4, the voltage modulated effective refractive index occurs primarily between the second non-conductive dielectric layer 12 and the third transparent conductive oxide layer 13. Considering that the formation of Ag nanowires is a gradual process, and the second non-conductive dielectric layer 12 can block the migration of Ag atoms, Ag accumulation layers with different thicknesses can be formed between the second non-conductive dielectric layer 12 and the third transparent conductive oxide layer 13 as the voltage application time increases. When no voltage is applied, the overall effective refractive index of the FP cavity is recorded as a. When a positive voltage is applied preliminarily, Ag in the third transparent conductive oxide layer 13 migrates to the second non-conductive dielectric layer 12 and is blocked at the interface of the second non-conductive dielectric layer 12 and the third transparent conductive oxide layer 13 to form an Ag accumulation layer with the thickness of 1nm, Ag nano-wires in the third transparent conductive oxide layer 13 are preliminarily formed at the moment, and under the action of the Ag accumulation layer, the whole effective refractive index of the FP cavity is changed, and the effective refractive index is b at the moment. With further application of positive voltage, the Ag nanowires in the third transparent conductive oxide layer 13 are further formed to form an Ag accumulation layer with a thickness of 2nm, and the overall effective refractive index of the FP cavity continues to change, at which time the effective refractive index is recorded as c. When a positive voltage is further applied, Ag in the third transparent conductive oxide layer 13 is completely formed into an Ag accumulation layer with a thickness of 3nm, and at this time, Ag nanowires in the third transparent conductive oxide layer 13 are completely formed, and the effective refractive index is recorded as d. After the reverse voltage is applied, the Ag nanowires of the third transparent conductive oxide layer 13 are gradually broken, and the effective refractive index is also restored to the initial value.
Fig. 5 shows the simulation result of FDTD (time domain effective difference method) according to the present invention, where the incident light is vertical.
When no positive voltage is applied to the FP cavity control unit, the Ag nanowire is not formed in the third transparent conductive oxide layer 13, and at this time, the effective refractive index corresponds to the curve shown by the effective refractive index a in fig. 5, the resonance peak position is 508.5nm, and the reflectivity is 0.04.
When the FP cavity control unit initially applies a positive voltage, Ag nanowires of the third transparent conductive oxide layer 13 are initially formed, corresponding to a curve shown by the effective refractive index b in fig. 5, whose resonance peak position is 558.7nm and whose reflectance is 0.12.
When the FP cavity control unit further applied a positive voltage, Ag nanowires of the third transparent conductive oxide layer 13 were further formed, corresponding to the curve shown by the effective refractive index c in fig. 5, whose resonance peak position was 633.1nm and whose reflectance was 0.01.
When the FP cavity control unit further applies a positive voltage, the Ag nanowire of the third transparent conductive oxide layer 13 is completely formed, and the resonance peak position is 705.5nm and the reflectance is 0.03 corresponding to the curve shown by the effective refractive index d in fig. 5.
When the FP chamber control unit applies negative voltage, the Ag nano-wires of the third transparent conductive oxide layer 13 are gradually broken, so that the adjustment and the memory of the resonance position and the resonance strength are realized, the adjustment effects of the plurality of FP chamber control units can be mutually superposed, and the adjustment effect of the whole device is more obvious and flexible.
The foregoing embodiments are merely illustrative of the principles and utilities of the present invention and are not intended to limit the invention. Any person skilled in the art can modify or change the above-mentioned embodiments without departing from the spirit and scope of the present invention. Accordingly, it is intended that all equivalent modifications or changes which can be made by those skilled in the art without departing from the spirit and technical spirit of the present invention be covered by the claims of the present invention.

Claims (8)

1.一种用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:从上至下依次包括第一层金属薄膜层(11)、第二层非导电电介质层(12)、第三层透明导电氧化物层(13)、第四层金属层(14)、第五层衬底层(15);1. A Fabry-Perot cavity filter for dynamic color regulation, characterized in that: from top to bottom, it comprises a first metal thin film layer (11), a second non-conductive dielectric layer (12) , a third transparent conductive oxide layer (13), a fourth metal layer (14), and a fifth substrate layer (15); 其中,所述第一层金属薄膜层(11)用于将入射光引入法布里-珀罗腔,并作为法布里-珀罗腔的金属-绝缘体-金属结构中的上层金属层;Wherein, the first metal thin film layer (11) is used to introduce incident light into the Fabry-Perot cavity, and is used as the upper metal layer in the metal-insulator-metal structure of the Fabry-Perot cavity; 所述第二层非导电电介质层(12)作为法布里-珀罗腔的金属-绝缘体-金属结构中的中间电介质层,并作为阻挡层阻挡介电常数趋于0的材料发生电化学金属化后的金属离子迁移;The second non-conductive dielectric layer (12) acts as an intermediate dielectric layer in the metal-insulator-metal structure of the Fabry-Perot cavity, and acts as a blocking layer to block the electrochemical metal generation of a material whose dielectric constant tends to zero. The migration of metal ions after chemical treatment; 所述第三层透明导电氧化物层(13)为介电常数趋于0的材料,在电场作用下能实现折射率的改变,从而调节法布里-珀罗腔腔体的折射率;The third transparent conductive oxide layer (13) is a material with a dielectric constant close to 0, which can change the refractive index under the action of an electric field, thereby adjusting the refractive index of the Fabry-Perot cavity; 所述第四层金属层(14)作为法布里-珀罗腔金属-绝缘体-金属结构中的下层金属层;The fourth metal layer (14) is used as the lower metal layer in the Fabry-Perot cavity metal-insulator-metal structure; 最下面为第五层衬底层(15),在衬底上制备上述结构;The bottom is the fifth substrate layer (15), and the above structure is prepared on the substrate; 同时,第一层金属薄膜层(11)、第二层非导电电介质层(12)、第三层透明导电氧化物层(13)和第四层金属层(14)构成忆阻单元,其中第一层金属薄膜层(11)作为第一电极,第四层金属层(14)作为第二电极,第一层金属薄膜层(11)和第二层非导电电介质层(12)形成相互垂直的交叉阵列结构,第二层非导电电介质层(12)和第三层透明导电氧化物层(13)形成相互垂直的交叉阵列结构,第一电极与第二电极电连接,对忆阻单元施加电压完成对折射率的调控,撤去电压,折射率完成记忆。At the same time, the first metal thin film layer (11), the second non-conductive dielectric layer (12), the third transparent conductive oxide layer (13) and the fourth metal layer (14) constitute a memristive unit, wherein the first layer A metal thin film layer (11) is used as a first electrode, a fourth metal film layer (14) is used as a second electrode, and the first metal thin film layer (11) and the second non-conductive dielectric layer (12) are formed to be perpendicular to each other. Cross-array structure, the second non-conductive dielectric layer (12) and the third transparent conductive oxide layer (13) form a cross-array structure perpendicular to each other, the first electrode is electrically connected to the second electrode, and a voltage is applied to the memristive unit After completing the regulation of the refractive index, the voltage is removed, and the refractive index is memorized. 2.根据权利要求1所述的用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:所述第一层金属薄膜层(11)为Au,Au膜厚度保证入射光能够穿过Au薄膜进入FP腔,Au膜厚度为15-30nm。2. The Fabry-Perot cavity filter for dynamic color control according to claim 1, wherein the first metal thin film layer (11) is Au, and the thickness of the Au film ensures that incident light can Enter the FP cavity through the Au thin film with a thickness of 15-30 nm. 3.根据权利要求1所述的用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:所述第二层非导电电介质层(12)为二氧化钛层,二氧化钛作为非导电电介质使忆阻单元形成电场,二氧化钛层厚度为50-100nm。3. The Fabry-Perot cavity filter for dynamic color control according to claim 1, wherein the second non-conductive dielectric layer (12) is a titanium dioxide layer, and titanium dioxide is used as a non-conductive dielectric The memristive cells are formed with an electric field, and the thickness of the titanium dioxide layer is 50-100 nm. 4.根据权利要求1所述的用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:所述第三层透明导电氧化物层(13)为二氧化硅掺银薄膜层,二氧化硅中预置的Ag掺杂体积分数为90%,二氧化硅掺银薄膜层存在介电常数实部区域0的区域,二氧化硅掺银薄膜层厚度为75-150nm。4. The Fabry-Perot cavity filter for dynamic color control according to claim 1, wherein the third transparent conductive oxide layer (13) is a silicon dioxide silver-doped thin film layer , the preset Ag-doped volume fraction in the silicon dioxide is 90%, the silicon dioxide silver-doped thin film layer has a region with a real part of the dielectric constant region 0, and the thickness of the silicon dioxide silver-doped thin film layer is 75-150nm. 5.根据权利要求1所述的用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:所述第四层金属层(14)为Au层,Au层厚度为200-300nm。5. The Fabry-Perot cavity filter for dynamic color control according to claim 1, wherein the fourth metal layer (14) is an Au layer, and the thickness of the Au layer is 200-300nm . 6.根据权利要求1所述的用于动态色彩调控的法布里-珀罗腔滤波器,其特征在于:所述第五层衬底层(15)为Si衬底层,其厚度为15mm。6 . The Fabry-Perot cavity filter for dynamic color control according to claim 1 , wherein the fifth substrate layer ( 15 ) is a Si substrate layer, and its thickness is 15 mm. 7 . 7.权利要求1至6任意一项所述的用于动态色彩调控的法布里-珀罗腔滤波器的制备方法,其特征在于包括如下步骤:7. the preparation method of the Fabry-Perot cavity filter described in any one of claim 1 to 6 for dynamic color regulation is characterized in that comprising the steps: (1)在第五层衬底层(15)上使用直流磁控溅射的方式沉积Au膜;(1) depositing an Au film on the fifth substrate layer (15) by means of DC magnetron sputtering; (2)在第四层金属层(14)上使用射频磁控共溅射的方式沉积二氧化硅掺银透明导电膜,使用掩模版对该层材料图形化;(2) depositing a silicon dioxide silver-doped transparent conductive film on the fourth metal layer (14) by means of radio frequency magnetron co-sputtering, and using a mask to pattern the layer material; (3)在第三层透明导电氧化物层(13)上使用直流磁控溅射的方式沉积二氧化钛,使用掩模版对该层材料图形化;(3) depositing titanium dioxide by means of DC magnetron sputtering on the third transparent conductive oxide layer (13), and patterning the layer material using a reticle; (4)在第二层非导电电介质层(12)上使用直流磁控溅射的方法沉积Ag薄膜,使用掩模版对该层材料图形化形成电极。(4) depositing an Ag thin film on the second non-conductive dielectric layer (12) by DC magnetron sputtering, and patterning the layer material with a mask to form electrodes. 8.权利要求4所述的用于动态色彩调控的法布里-珀罗腔滤波器的共振波长和共振强度的调谐方法,其特征在于包括如下步骤:8. the tuning method of the resonance wavelength and the resonance intensity of the Fabry-Perot cavity filter that is used for dynamic color regulation and control according to claim 4, is characterized in that comprising the steps: 在未施加电压的时候,滤波器对x1波长具有强烈的吸收,呈现出a颜色,通过电压装置对第四层金属层(14)施加正电压,第三层透明导电氧化物层(13)中Ag原子会发生电化学金属化,由于第三层透明导电氧化物层中预埋了Ag,相邻的Ag团簇相当于两个电极,Ag原子通过氧化还原反应会在Ag团簇之间会形成Ag纳米丝,导致第三层透明导电氧化物层的有效折射率发生变化,靠近第二层非导电电介质层和第三层透明导电氧化物层的界面处的Ag纳米丝形成会被阻挡在界面处,形成一层Ag层,此时第三层透明导电氧化物层的折射率随着Ag纳米丝的形成,折射率发生改变,对x2波长具有强烈的吸收,呈现出b颜色;随着进一步对第四层金属层施加正电压,第三层透明导电氧化物层中的Ag纳米丝进一步形成,折射率继续发生改变,此时对x3波长具有强烈的吸收,呈现出c颜色;When no voltage is applied, the filter has strong absorption for x 1 wavelength, showing a color, and a positive voltage is applied to the fourth metal layer (14) through the voltage device, and the third transparent conductive oxide layer (13) The Ag atoms in the middle will undergo electrochemical metallization. Since Ag is pre-buried in the third transparent conductive oxide layer, the adjacent Ag clusters are equivalent to two electrodes, and the Ag atoms will be between the Ag clusters through the redox reaction. Ag nanowires will form, resulting in a change in the effective refractive index of the third transparent conductive oxide layer, and the formation of Ag nanowires near the interface of the second non-conductive dielectric layer and the third transparent conductive oxide layer will be blocked At the interface, a layer of Ag is formed. At this time, the refractive index of the third transparent conductive oxide layer changes with the formation of Ag nanowires, and has strong absorption for x2 wavelength, showing b color; As a positive voltage is further applied to the fourth metal layer, Ag nanowires in the third transparent conductive oxide layer are further formed, and the refractive index continues to change. At this time, it has strong absorption for x3 wavelength, showing c color ; 通过电压装置对第一层金属薄膜层(11)施加正电压,Ag原子继续发生电化学金属化效应,第三层透明导电氧化物层的Ag纳米丝开始逐渐断裂,折射率发生变化,对x2波长具有强烈的吸收,呈现出b颜色,随着进一步对第一层金属薄膜层(11)施加正电压,第三层透明导电氧化物层中形成的Ag丝完全断裂,折射率回到初始值,对x1波长具有强烈的吸收,呈现出a颜色。A positive voltage is applied to the first metal thin film layer (11) through a voltage device, the Ag atoms continue to undergo electrochemical metallization effect, the Ag nanowires of the third transparent conductive oxide layer begin to break gradually, and the refractive index changes, and the x 2 wavelengths have strong absorption, showing b color, with the further application of positive voltage to the first metal thin film layer (11), the Ag filament formed in the third transparent conductive oxide layer is completely broken, and the refractive index returns to the original value, with strong absorption at x 1 wavelength, showing a color.
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