CN106444214A - Kerr defect-containing cosine function type photonic crystal low-threshold optical bistable device - Google Patents

Kerr defect-containing cosine function type photonic crystal low-threshold optical bistable device Download PDF

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CN106444214A
CN106444214A CN201610910208.6A CN201610910208A CN106444214A CN 106444214 A CN106444214 A CN 106444214A CN 201610910208 A CN201610910208 A CN 201610910208A CN 106444214 A CN106444214 A CN 106444214A
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defect
photonic crystal
kerr
function type
layer
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王筠
刘丹
吉紫娟
靳海芹
李建明
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Hubei University of Education
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Hubei University of Education
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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
    • G02F3/00Optical logic elements; Optical bistable devices
    • G02F3/02Optical bistable devices
    • G02F3/024Optical bistable devices based on non-linear elements, e.g. non-linear Fabry-Perot cavity

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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 discloses a Kerr defect-containing cosine function type photonic crystal low-threshold optical bistable device. Low-threshold optical bistability is realized by mutually coupling two semifinite photonic crystals (BA)m and (AB)m composed of two cosine function refractive index medium layers (A and B) alternatively and a center layer D made of a Kerr nonlinear defect material. Compared with the conventional photonic crystal optical bistable device, the photonic crystal low-threshold optical bistable device disclosed by the invention has the characteristics of low threshold and subminiature, can be applied to optical switches, optical storage and other occasions of optical communication and integrated optical circuits. The center layer D is a Kerr defect symmetrical cosine function type photonic crystal low-threshold optical bistable device and is capable of realizing coupled integration of other integrated optical circuit devices.

Description

The cosine function type photonic crystal Low threshold optical bistable device of defect containing Kerr
Technical field
The present invention relates to the all-optical switch in quantum calculation and quantum communication, all-optical storage, full optical transistor and full light to patrol Collect the technical fields such as circuit, specifically for one defect containing Kerr cosine function type photonic crystal Low threshold optical bistable device.
Background technology
Since Yablonovitch and John in 1987 proposes the concept of photonic crystal, photonic crystal has become photoelectricity One important research field of sub-material.Photonic crystal is the periodic dielectric structures prepared according to symmetry of crystals, its electricity Magnetic pattern has band structure as the electronic state in crystal.The energy band of photonic crystal is by the symmetry of photonic crystal, component The size of the dielectric function of material and primitive unit cell determines.The size of dielectric function or change primitive unit cell by changing material, can adjust The position of photonic band gap processed and width.Particularly under one-dimensional case, the band gap of photonic crystal is readily changed by being situated between Electric constant or geometry or doping are modulated.Generally, dielectric constant or the refractive index of photon crystal material are formed For constant, the position of its band gap and the width of band gap are fixing;If adding nonlinear dielectric layer wherein, reform into as supporting by the arm Miscellaneous non-linear photon crystal, can realize optical bistability.In general photonic crystal, normal optical bistable state utilizes belt edge Dynamic mobile realizes, and mixes up photonic crystal and be by mean of the dynamic mobile of Defect Modes and realize dispersed light bistable.Correlative study Showing, 1-D photon crystal may be used for controlling the system of optical bistability, i.e. only need to be close to the other increasing of non-linear photon crystal Add additional coatings such as phase matching layer, negative index layer or sub-wavelength layer, it is possible to control optical bistability.Therefore, mix up one-dimensional Photonic crystal is considered as the system that can make compact optical device.
Have document to propose the concept of a kind of novel function photonic crystal, the dielectric layer refractive index of this photonic crystal be with The periodic function of spatial position change, light wave is propagated along curved path wherein.Research discovery, in order to obtain this kind of photonic crystal More broad-band gap can be realized by adding suitable defect layer;And the impact that the dispersion of defect is on this kind of photonic crystal photon band gap It is also to be worth further investigation.
We utilize transfer matrix method and use Lorenz oscillator model to dispersion defect layer recently, have studied one-dimensional containing look Dissipating Sinc function type photonic crystal forbidden photon band and the dispersion Defect Modes of defect, discovery can obtain broad photon after adding defect Forbidden band, tunnelling Defect Modes frequency band is narrow and neighbouring field distribution height local.If it is brilliant that NONLINEAR DEFECT is introduced function type photon In body, it is anticipated that while obtaining extremely broad forbidden photon band, realize optical bistability by the corresponding parameter of regulation, this The Defect Modes frequency band being because in forbidden band is narrow, and the mode of electromagnetic wave density of states at Defect Modes frequency is very big, by highly beneficial Generation in nonlinear effect.
Content of the invention
In view of this, present invention is primarily targeted at provide a kind of be suitable for integreted phontonics, brilliant by function type photon The cosine function type photonic crystal Low threshold optical bistable device that body and non-linear microcavity are combined into.
For reaching above-mentioned purpose, the invention provides a kind of cosine function type photonic crystal Low threshold light of defect containing Kerr double Steady device, this contains Kerr defect function type photonic crystal is to be made up of central core, the left and right sides Kerr NONLINEAR DEFECT layer D by remaining String function index dielectric layer A, B replace two and half limited photonic crystals (BA) of compositionm(AB)mSymmetric periodic structure (BA)mD(AB)m, wherein m is periodicity.
In said structure, the relational expression that A, medium B layer refractive index are changed by cosine function with locus isThe thickness of dielectric layer A and B It is respectively dA=a, dB=b, both meetsWherein λ0And ω0It is incident light respectively The centre wavelength of ripple and center circle frequency.
Said structure, the index of refraction relationship formula of center NONLINEAR DEFECT layer D isWhereinFor linear refractive index, unrelated with light intensity;χ(3)For its three rank electric susceptibility;Microcavity length dDMeet
In said structure, each parameter value is n respectivelyA(0)=3.37, nB(0)=1.544, A1=0.2, A2=0.1, a= 221.388nm, b=483.211nm, the thickness of dielectric layer A is dA=221.388nm, the thickness of dielectric layer B is dB= 483.211nm;The linear refractive index of defect layer DThree rank electric susceptibilities χ(3)=2.5 × 10-12m2·V-2, its thickness It is dD=373.039nm.
In such scheme, light wave incidence angle θ=π/12, incidence wave center circle frequency is
Beneficial effects of the present invention:
1. the central core that the present invention provides is the symmetrical cosine function type photonic crystal Low threshold optical bistability of Kerr defect, profit With the two and half limited photonic crystals (BA) being alternately made up of two cosine functions index dielectric layer A, Bm(AB)mWith by The central core D that Kerr NONLINEAR DEFECT material is constituted intercouples and realizes Low threshold optical bistability.
2. the central core that the present invention provides is the symmetrical cosine function type photonic crystal Low threshold optical bistability of Kerr defect, with Conventional photonic crystal optical bistability compares and has lower-threshold and subminiature feature, can be applicable to optic communication and integrated optical circuit Photoswitch, the occasion such as optical storage.
3. present invention focuses primarily on the non-linear microcavity of Kerr respectively with both sides around by cosine function index medium Layer A, B replace two and half limited photonic crystals (BA) of compositionm(AB)mBe coupled the lower-threshold realizing in light wave frequency range Bistable research, the central core studied is that the symmetrical cosine function type photonic crystal Low threshold optical bistability of Kerr defect can be real The now coupling integration with other multifunction integrated optical circuit device.
Brief description
Fig. 1 be central core be the symmetrical cosine function type photonic crystal Low threshold optical bistability structural representation of Kerr defect.
Fig. 2 is less at incident intensity, and in defect layer D, nonlinear effect is negligible, and D is equivalent to a linear discontinuities layer.
Fig. 3 is the central linear tunnelling mode ω of cosine function type photonic crystal Fig. 2m1=1.0029 ω0Near bistable state, Multistable curve.
Fig. 4 is periodic structure (BA)5D(AB)5Bistable state threshold near the tunnelling mode of respective center for the longitudinal cosine type photonic crystal Value is with the linear refractive index of non-linear microcavity DTake respectively the 2nd, the 3rd, 4 when variation tendency, in Fig. 4, red data point represents high threshold Value, black data point represents Low threshold.
Fig. 5 is periodic structure (BA)5D(AB)5Sinc type photonic crystal heart tunnelling mode ω whereinm=0.9949 ω0Attached Near bistable threshold is with the linear refractive index of non-linear microcavity DTake respectively the 2nd, the 3rd, 4 when variation tendency.
Detailed description of the invention
For making the object, technical solutions and advantages of the present invention clearer, below in conjunction with specific embodiment, and reference Accompanying drawing, the present invention is described in more detail.
Fig. 1 be central core be the symmetrical cosine function type photonic crystal Low threshold optical bistability structural representation of Kerr defect.
Fig. 2 is less at incident intensity, and in defect layer D, nonlinear effect is negligible, and D is equivalent to a linear discontinuities layer. It is fixed to take in Fig. 1When, periodicity m take respectively the 5th, the 6th, 7 when cosine function type photonic crystal different cycles number transmission spectrum, In (a), (b) and (c) of Fig. 1, three linear tunnelling modes are ω respectivelym1=0.9805 ω0、ωm2=1.0029 ω0、ωm3= 1.025ω0;Calculate and also find, whenTake respectively the 2nd, the 3rd, 4 when, also have a collinearity tunnelling mode ωm=1.0029 ω0.
Fig. 3 is the central linear tunnelling mode ω of cosine function type photonic crystal Fig. 2m1=1.0029 ω0Near bistable state, Multistable curve.
Fig. 4 is periodic structure (BA)5D(AB)5Bistable state threshold near the tunnelling mode of respective center for the longitudinal cosine type photonic crystal Value is with the linear refractive index of non-linear microcavity DTake respectively the 2nd, the 3rd, 4 when variation tendency.
Fig. 5 is periodic structure (BA)5D(AB)5Sinc type photonic crystal heart tunnelling mode ω whereinm=0.9949 ω0Attached Near bistable threshold is with the linear refractive index of non-linear microcavity DTake respectively the 2nd, the 3rd, 4 when variation tendency.A, medium B layer folding Rate of penetrating is distributed to be respectivelyWith The thickness of dielectric layer A and B is respectively dA=(p-q)/2=a, dB=(p+q)/2=b, the two is also satisfied
In the present embodiment, the Low threshold optical bistable device of a kind of function type photonic crystal of defect containing Kerr, this contains Kerr and lacks Falling into function type photonic crystal is to be constituted central core, the left and right sides by cosine function index medium by Kerr NONLINEAR DEFECT layer D Layer A, B replace two and half limited photonic crystals (BA) of compositionm(AB)mSymmetric periodic structure (BA)mD(AB)m, wherein m is Periodicity.
The central core that the present invention provides is the symmetrical cosine function type photonic crystal Low threshold optical bistability structure of Kerr defect Schematic diagram, as it is shown in figure 1, this example takes periodicity m=5, uses two kinds of different cosine function index dielectric layer A, B, it Refractive index with the change profile formula of locus coordinate z be respectively:
Wherein nA(0)=3.37, nB(0)=1.544, A1=0.1, A2=0.2, a=221.388nm, b=483.211nm, is situated between The thickness of matter layer A, B is d respectivelyA=a=221.388nm, dB=b=483.211nm, A, medium B layer optical thickness meetThe half limited photonic crystal (BA) being made up of them5(AB)5It is positioned at central core D Both sides, z-axis is perpendicular to this photonic crystal interface, as shown in Figure 1;Central core D is be made up of Kerr nonlinear dielectric micro- Chamber, this Kerr nonlinear dielectric refractive index isWhereinFor linear refractive index, with light intensity without Closing, three rank electric susceptibilities are c(3)=2.5 × 10-12m2V-2, EDZ () is the electric-field intensity in microcavity at z;Microcavity length dDMeetIncident light wave center circle frequency w0=6.313016 × 1014Rad/s, light wave incidence angle is θ=π/12.
Being known by Fig. 3, Fig. 4, the cosine function type photonic crystal of defect containing Kerr realizes bistable incident light wave frequency distribution Be centrifugal pump, i.e. this structure only could realize bistable state at specific frequency.Low threshold bistable state to be obtained, at defect layer D Under conditions of optical thickness is constant, the linear refractive index of nonlinear materialValue is lower realizes that bistable threshold value is lower.
The central core that the present invention provides is that the symmetrical cosine function type photonic crystal Low threshold optical bistability of Kerr defect has Subminiature feature.The central core that can be obtained this example by the above-mentioned concrete data providing provides is the symmetrical cosine of Kerr defect Function type photonic crystal Low threshold optical bistability total optical thickness along the z-axis direction is 16.41370632mm.
When incident intensity is less, the nonlinear effect in defect layer D is negligible, and D is equivalent to a linear discontinuities layer.By In the periodicity close relation of periodic structure transmissivity and periodic structure, fixed takingWhen, periodicity m=n takes respectively 5th, the 6th, 7 when the type of cosine function containing defect, wherein in (a), (b) and (c) in Fig. 1, three linear tunnelling modes are all:ωm1= 0.9805ω0、ωm2=1.0029 ω0、ωm3=1.025 ω0, as shown in Figure 2.Frequency characteristic due to periodic structure containing defect Very tight with defect layer index of refraction relationship, calculate discovery:WhenTake respectively the 2nd, the 3rd, 4 when, longitudinal cosine type photonic crystal has one altogether Collinearity tunnelling mode ωm=1.0029 ω0, this is also the center tunnelling mode of Fig. 2.
When incident intensity is bigger, the nonlinear effect of defect layer D is obvious, and D becomes non-linear microcavity, now output intensity With input light Qianghian relation curve, as it is shown on figure 3, Fig. 3 is given be cosine function type photonic crystal Fig. 2 (c) in The heart linear tunnelling mode ωm1=1.0029 ω0Near bistable state, multistable curve.From formula (3), non-linear microcavity D infolding Penetrate rate nDBecoming the increase with light intensity big, its relative dielectric constant also becomes big, it is possible to resultant field reduces in causing D, Nonlinear effect will weaken, it is achieved bistable threshold value is possible to nDIncrease and become big.Calculate further and show, identical Under the premise of periodic structure, when A, medium B layer refractive index remainder string functional form relatively takes Sinc functional form when bistable threshold Lower, as shown in Figure 4 and Figure 5.Correlative study is it is also shown that the more conventional photonic crystal of Sinc function type photonic crystal bistable threshold Low.
These are only some embodiments of the present invention, to those skilled in the art, without departing from this On the premise of bright creation design, also can carry out some deformation and improve, these broadly fall into protection scope of the present invention.

Claims (6)

1. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr, it is characterised in that this contains Kerr defect Function type photonic crystal is to be constituted central core, the left and right sides by cosine function index dielectric layer by Kerr NONLINEAR DEFECT layer D A, B replace two and half limited photonic crystals (BA) of compositionm(AB)mSymmetric periodic structure (BA)mD(AB)m, wherein m is week Issue.
2. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr according to claim 1, its feature exists In the relational expression that A, medium B layer refractive index are changed by cosine function with locus is WithThe thickness of dielectric layer A and B is respectively dA=a, dB=b, both meetsWherein λ0And ω0It is centre wavelength and the center circle frequency of incident light wave respectively.
3. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr according to claim 1, its feature exists In defect layer D is the nonlinear dielectric with Kerr effect, and the index distribution of Kerr medium isWhereinFor linear refractive index, unrelated with light intensity;χ(3)For its three rank electric susceptibility;ED(z) It is the electric-field intensity in defect layer at z;Microcavity length dDMeet
4. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr according to Claims 2 or 3, its feature Being, parameter value is respectively:nA(0)=3.37, nB(0)=1.544, A1=0.2, A2=0.1, a=221.388nm, b= 483.211nm, then the thickness of dielectric layer A is dA=221.388nm, the thickness of dielectric layer B is dB=483.211nm;Defect layer D Linear refractive indexThree rank electric susceptibilities χ(3)=2.5 × 10-12m2·V-2, its thickness is dD=373.039nm; Light wave incidence angle θ=π/12, incidence wave center circle frequency
5. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr according to claim 3, its feature exists In when incident intensity is less, the nonlinear effect in defect layer D is negligible, and defect layer D is a linear discontinuities layer;Cycle Structure transmissivity and the periodicity close relation of periodic structure, determine when takingWhen, periodicity m take respectively the 5th, the 6th, 7 when contain Defect cosine function type photonic crystal (BA)mD(AB)mHave three linear tunnelling modes:ωm1=0.9805 ω0、ωm2= 1.0029ω0、ωm3=1.025 ω0;WhenTake respectively the 2nd, the 3rd, 4 when, longitudinal cosine type photonic crystal has a collinearity tunnelling mode ωm=1.0029 ω0.
6. the Low threshold optical bistable device of the function type photonic crystal of defect containing Kerr according to claim 3, its feature exists In refractive index n in defect layer DDBecoming the increase with light intensity big, its relative dielectric constant also becomes big, resultant field in defect layer D Reducing, nonlinear effect will weaken, it is achieved bistable threshold value is with refractive index nDIncrease and become big.
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761639A (en) * 2018-05-02 2018-11-06 上海大学 A kind of photonic crystal all-optical diode
CN109298583A (en) * 2018-12-06 2019-02-01 湖北科技学院 One kind being based on the bistable all-optical switch of graphene optical and optical memory
CN109669227A (en) * 2019-02-27 2019-04-23 湖北科技学院 A kind of photonic crystal of pair of Defect Modes reflectivity enhancing
CN111505757A (en) * 2020-06-02 2020-08-07 中国人民解放军火箭军工程大学 Infrared and laser compatible camouflage film system structure utilizing symmetric center defect

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104280152A (en) * 2014-09-03 2015-01-14 上海大学 Dynamic tuning type temperature sensor
CN105629623A (en) * 2015-06-24 2016-06-01 上海大学 Tunable temperature bistable optical switch
CN105739135A (en) * 2016-03-25 2016-07-06 南京邮电大学 Magneto-optic isolator prepared from metamaterial with low dielectric constant

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104280152A (en) * 2014-09-03 2015-01-14 上海大学 Dynamic tuning type temperature sensor
CN105629623A (en) * 2015-06-24 2016-06-01 上海大学 Tunable temperature bistable optical switch
CN105739135A (en) * 2016-03-25 2016-07-06 南京邮电大学 Magneto-optic isolator prepared from metamaterial with low dielectric constant

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
王筠等: "Sinc函数型光子晶体非线性微腔的光学双稳态", 《激光与光电子学进展》 *
王筠等: "含色散负折射率缺陷一维Sinc函数型光子晶体的光学传输特性", 《中国激光》 *
邓开发等: "含缺陷态的非线性介质材料的光子晶体的双稳态特性", 《激光杂志》 *
黄晓琴等: "掺杂非线性吸收介质的光子晶体的双稳态特性", 《光电子·激光》 *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761639A (en) * 2018-05-02 2018-11-06 上海大学 A kind of photonic crystal all-optical diode
CN109298583A (en) * 2018-12-06 2019-02-01 湖北科技学院 One kind being based on the bistable all-optical switch of graphene optical and optical memory
CN109298583B (en) * 2018-12-06 2021-07-20 湖北科技学院 All-optical switch and optical memory based on graphene optical bistable state
CN109669227A (en) * 2019-02-27 2019-04-23 湖北科技学院 A kind of photonic crystal of pair of Defect Modes reflectivity enhancing
CN109669227B (en) * 2019-02-27 2024-04-05 湖北科技学院 Photonic crystal with enhanced reflectivity to defect mode
CN111505757A (en) * 2020-06-02 2020-08-07 中国人民解放军火箭军工程大学 Infrared and laser compatible camouflage film system structure utilizing symmetric center defect
CN111505757B (en) * 2020-06-02 2022-03-01 中国人民解放军火箭军工程大学 Infrared and laser compatible camouflage film system structure utilizing symmetric center defect

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