CN110797747A - Laser transmitter based on all-dielectric super surface and parameter determination method - Google Patents
Laser transmitter based on all-dielectric super surface and parameter determination method Download PDFInfo
- Publication number
- CN110797747A CN110797747A CN201911075885.0A CN201911075885A CN110797747A CN 110797747 A CN110797747 A CN 110797747A CN 201911075885 A CN201911075885 A CN 201911075885A CN 110797747 A CN110797747 A CN 110797747A
- Authority
- CN
- China
- Prior art keywords
- mirror
- silicon cylindrical
- reflector
- silicon
- laser
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/02—Structural details or components not essential to laser action
- H01S5/028—Coatings ; Treatment of the laser facets, e.g. etching, passivation layers or reflecting layers
- H01S5/0285—Coatings with a controllable reflectivity
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
- H01S5/18—Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities
- H01S5/185—Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only horizontal cavities, e.g. horizontal cavity surface-emitting lasers [HCSEL]
- H01S5/187—Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only horizontal cavities, e.g. horizontal cavity surface-emitting lasers [HCSEL] using Bragg reflection
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Semiconductor Lasers (AREA)
Abstract
The invention discloses a laser transmitter based on an all-dielectric super surface. The laser emitter comprises the following components in sequence from bottom to top: a first mirror, an active layer, and a second mirror; the first reflecting mirror and the second reflecting mirror are each composed of periodically arranged silicon cylindrical particles. The first reflector and the second reflector of the invention greatly reduce the thickness of the reflector and effectively reduce the whole volume of the laser emitter by adopting the structure of silicon cylindrical particles which are periodically arranged.
Description
Technical Field
The invention relates to the technical field of computational electromagnetic metamaterials and multi-physics simulation, in particular to a laser transmitter based on an all-dielectric super surface and a parameter determination method.
Background
The super surface is a two-dimensional sheet-like metamaterial, and the thickness of the super surface is several times smaller than the working wavelength. Their subwavelength structures propagate in a two-dimensional space in a periodic or non-periodic manner. The super-surface can be used to provide special optical properties to the device that some natural material films cannot achieve. In recent years, all-dielectric metamaterials and metamaterials have been considered to be more efficient counterparts to plasmonic materials. The core principle of all-dielectric metamaterials and metamaterials is the optical response of high-index-of-refraction dielectric nanoparticles. At present, because of the existence of electric resonance and magnetic resonance in the visible light range, the dielectric nanoparticles with high refractive index can effectively control light scattering and strength enhancement, and have the advantages of negligible extinction coefficient and extremely low loss. The all-dielectric super-surface is applied to the fields of wavefront engineering, electromagnetic induction transparency, high transmittance, broadband perfect mirrors, beam collimators and the like, particularly the broadband perfect mirrors, and provides a new unique opportunity for designing optical lenses, particularly semiconductor laser resonators.
The semiconductor laser has the advantages of small size, high efficiency, long service life, easy integration and the like. The semiconductor laser with high beam quality and narrow linewidth has higher beam quality, smaller slow axis divergence angle and narrower spectral linewidth, and is more suitable for shaping and combining large-scale semiconductor laser. Has wider application prospect in the aspects of industry, military, medical treatment and the like. The production of high power, high beam quality, narrow linewidth semiconductor lasers has been a goal of pursuit. However, although the conventional laser with the distributed bragg grating structure has the characteristic of easy operation in terms of preparation process and design, in the conventional distributed bragg reflector, a reflector is composed of a layer of high-refractive-index medium and a layer of low-refractive-index medium alternately, and incident light enters a dielectric layer and is reflected layer by the dielectric layer. Therefore, the method of controlling the reflectivity of the mirror in the bragg reflector is to increase or decrease the number of the reflective layers of the entire period, which is very inconvenient for controlling the thickness of the mirror and the size of the laser.
Disclosure of Invention
The invention aims to provide a laser transmitter based on an all-dielectric super-surface and a parameter determination method, which greatly reduce the thickness of a reflector and effectively reduce the overall volume of the laser transmitter.
In order to achieve the purpose, the invention provides the following scheme:
a laser transmitter based on a full-medium super surface,
the laser emitter comprises the following components in sequence from bottom to top: a first mirror, an active layer, and a second mirror;
the first reflecting mirror and the second reflecting mirror are each composed of periodically arranged silicon cylindrical particles.
Optionally, the laser transmitter further includes: a first confinement layer and a second confinement layer;
the first confinement layer is disposed between the first mirror and the active layer; the second confinement layer is disposed between the active layer and the first mirror; the first limiting layer and the second limiting layer are used for limiting carriers and adjusting resonance wavelength to enable the resonance wavelength to be equal to laser wavelength.
Optionally, the laser transmitter further includes: a substrate;
the first mirror the substrate is located below the first mirror.
Optionally, the laser transmitter further includes: a first metal contact layer and a second metal contact layer;
the first metal contact layer is positioned below the substrate and is in ohmic contact with the substrate;
the second metal contact layer is located on the second mirror, and the second metal contact layer is in ohmic contact with the second mirror.
Optionally, trivalent elements are doped into the silicon cylindrical particles of the first reflector; and pentavalent elements are doped into the silicon cylindrical particles of the second reflector.
Optionally, a light outlet is correspondingly formed on the second reflector and the second metal contact layer respectively; the light outlet is used for outputting laser beams.
Optionally, the active layer comprises a plurality of quantum well layers.
Optionally, a gain medium is filled between the quantum well layers.
A parameter determination method of a silicon cylindrical particle applied to a laser emitter, the parameter determination method comprising:
determining the diameter of silicon cylindrical particles of the reflector according to the working wavelength of the laser;
determining the aspect ratio of the silicon cylindrical particles when the reflectivity of the reflector is the preset reflectivity through an experiment;
determining the thickness of the silicon cylindrical particles of the reflector according to the aspect ratio and the diameter of the silicon cylindrical particles;
obtaining a relation curve diagram of the reflectivity of the reflecting mirror and the period of the silicon cylindrical particle arrangement and a relation curve diagram of the modulation bandwidth of the reflecting mirror and the period of the silicon cylindrical particle arrangement through experiments;
determining the period range of the silicon cylindrical particle arrangement when the reflectivity of the reflector is a preset reflectivity according to a relation curve graph of the reflectivity of the reflector and the period of the silicon cylindrical particle arrangement;
and determining the period of the silicon cylindrical particle arrangement when the reflectivity of the reflector is a preset reflectivity according to a relation line graph of the modulation bandwidth of the reflector and the period of the silicon cylindrical particle arrangement.
Optionally, the determining the thickness of the silicon cylindrical particle of the mirror according to the aspect ratio and the diameter of the silicon cylindrical particle includes:
according to the aspect ratio and the diameter of the silicon cylindrical particles, using a formulaCalculating to obtain the thickness of the silicon cylindrical particles of the reflector;
wherein, αiAspect ratio of silicon cylindrical particles, S, as a mirroriThickness of silicon cylindrical particle as mirror, DiThe diameter of the silicon cylinder particle, i-1 or i-2, of the mirror, which is the first mirror when i-1,when i is 2, the mirror is a second mirror.
According to the specific embodiment provided by the invention, the invention discloses the following technical effects:
the first reflector and the second reflector in the laser emitter provided by the invention are both of periodically arranged silicon cylindrical particle structures, and the periodically arranged silicon cylindrical particles have high reflectivity and nanoscale thickness, so that the thickness of the reflector in the laser emitter is greatly reduced on the premise of ensuring the high reflectivity, and the overall volume of the laser emitter is effectively reduced.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings needed to be used in the embodiments will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art to obtain other drawings without inventive exercise.
FIG. 1 is a block diagram of a laser transmitter provided by the present invention;
FIG. 2 is a block diagram of a mirror provided by the present invention;
FIG. 3 is a plan view of a reflector provided by the present invention;
FIG. 4 is a diagram illustrating the relationship between the reflectivity of the mirror and the frequency of the mirror according to the present invention;
FIG. 5 is a schematic diagram of the relationship between reflectivity and aspect ratio provided by the present invention;
FIG. 6 is a graph of reflectivity versus period provided by the present invention;
FIG. 7 is a line graph of bandwidth versus period provided by the present invention;
FIG. 8 is a schematic diagram of a four-level system provided by the present invention;
FIG. 9 is a diagram illustrating the relationship between the quality factor and the wavelength of a conventional DBG laser transmitter;
FIG. 10 is a diagram illustrating the relationship between the quality factor and the wavelength of a laser transmitter according to the present invention;
FIG. 11 is a laser time domain diagram of a laser transmitter provided by the present invention;
FIG. 12 is a frequency domain plot corresponding to FIG. 11;
description of the symbols: 1-first mirror, 2-second mirror, 3-active layer, 4-substrate, 5-first confinement layer, 6-second confinement layer, 7-first metal contact layer, 8-second metal contact layer.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
The invention aims to provide a laser transmitter based on an all-dielectric super-surface and a parameter determination method, which greatly reduce the thickness of a reflector and effectively reduce the overall volume of the laser transmitter.
In order to make the aforementioned objects, features and advantages of the present invention comprehensible, embodiments accompanied with figures are described in further detail below.
The embodiment of the invention provides a laser transmitter based on an all-dielectric super surface, which sequentially comprises the following components from bottom to top: a first mirror 1, an active layer 3 and a second mirror 2. Preferably, the Laser transmitter is a VCSEL (Vertical Cavity Surface Emitting Laser).
As shown in fig. 2, the first mirror 1 and the second mirror 2 are each composed of periodically arranged silicon cylindrical particles; preferably, the reflectivity of the first mirror 1 is almost 100%; the reflectivity of the second mirror 2 is between 99% and 100%, as shown in fig. 4, the first and second mirrors constituting the output coupler. The diameter and period of the silicon cylindrical particle of the first reflector 1 and the silicon cylindrical particle of the second reflector 2 are the same, and the thickness of the silicon cylindrical particle of the second reflector 2 is greater than the thickness of the silicon cylindrical particle of the first reflector 1, wherein the period refers to the distance a (shown in fig. 3) between the central axes of two adjacent silicon cylindrical particles, and the diameter and period of the silicon cylindrical particle, the thickness of the silicon cylindrical particle of the first reflector 1 and the thickness of the silicon cylindrical particle of the second reflector 2 are determined according to the following method, specifically comprising:
determining the diameter of the silicon cylindrical particles according to the working wavelength of the laser; preferably, the working wavelength of the laser is 1500 nm; electric resonance is a basis for laser emitters capable of generating laser light, and the prior art has been disclosedGenerating electric resonance, wherein lambda is the working wavelength, and D is the diameter of the silicon cylindrical particle; in the embodiment of the present application, the silicon cylindrical particles of the reflector are periodically arranged, when the silicon cylindrical particles are periodically arranged, the obtained reflector resonates at a wavelength higher than that of a single silicon cylindrical particle, and experimental simulation shows that when the diameter of the silicon cylindrical particle of the reflector is 400nm, electrical resonance is generated.
The aspect ratio at which the reflectance is the preset reflectance is determined through experiments, as shown in fig. 5.
Determining the thickness of the silicon cylindrical particle of the mirror according to the aspect ratio and the diameter of the silicon cylindrical particle, comprising: using the formula of diameter and aspect ratio of silicon cylindrical particles
Calculating to obtain the thickness of the silicon cylindrical particle, wherein αiAspect ratio of silicon cylindrical particles, S, as a mirroriThickness of silicon cylindrical particle as mirror, DiThe diameter of the silicon cylinder particle is 1 or 2, and when 1, the mirror is the first mirror 1, and when 2, the mirror is the second mirror 2.
Graphs of the reflectance of the mirror with respect to the period of the silicon cylindrical particle arrangement and line graphs of the modulation bandwidth of the mirror with respect to the period of the silicon cylindrical particle arrangement were obtained through experiments, as shown in fig. 6 and 7.
Determining the periodic range of the silicon cylindrical particle arrangement when the reflectivity of the reflector is a preset reflectivity according to a relation curve graph of the reflectivity of the reflector and the period of the silicon cylindrical particle arrangement; when the reflectivity of the reflector is close to 1, the period range is 630-660 nm.
Determining the period of the silicon cylindrical particle arrangement when the reflectivity of the reflector is the preset reflectivity according to a relation line graph of the modulation bandwidth of the reflector and the period of the silicon cylindrical particle arrangement; when the period is 630nm, the bandwidth is much larger than the other bandwidths, and therefore, the period width is selected to be 630 nm.
The laser transmitter further includes: a first confinement layer 5 and a second confinement layer 6; a first confinement layer 5 is arranged between the first mirror 1 and the active layer 3; the second confinement layer 6 is arranged between the active layer 3 and the first mirror 1; the first confinement layer 5 and the second confinement layer 6 serve to confine carriers and to adjust the resonance wavelength to be equal to the laser wavelength.
The laser transmitter further includes: a substrate 4; the first mirror 1 is located between the active layer 3 and the substrate 4.
The laser transmitter further includes: a first metal contact layer 7 and a second metal contact layer 8; the first metal contact layer 7 is arranged at the bottom of the laser emitter, the first metal contact layer 7 is in contact with the substrate 4, and the first metal contact layer 7 is in ohmic contact with the substrate 4; the second metal contact layer 8 is arranged on top of the laser emitter, the second metal contact layer 8 is in contact with the second mirror 2, and the second metal contact layer 8 is in ohmic contact with the second mirror 2.
Trivalent elements are doped into silicon cylindrical particles of the first reflector 1, and the first reflector 1 is an n-type reflector based on a full-medium super surface; the second reflector 2 is a p-type all-dielectric super-surface based reflector, and pentavalent elements are doped in the silicon cylindrical particles of the second reflector 2.
A light outlet is correspondingly arranged on the second reflector 2 and the second metal contact layer 8 respectively; the light outlet is used for outputting laser beams. Preferably, the light outlet is a circular light outlet and outputs a circular laser beam.
The active layer 3 includes a plurality of quantum well layers. Preferably, the active layer 3 is composed of 1 to 3 quantum wells.
The gain medium is filled among the quantum well layers, the gain medium is described by a universal four-level system in simulation, and the simulation method is FDTD (Finite-Difference Time-Domain). For isotropic media, the expression of maxwell's equations in the time domain is as follows:
wherein, B ═ mu0H represents magnetic induction, mu represents magnetic permeability, mu0Denotes the permeability in vacuum, the intensity of the magnetic field H, the intensity of the electric field E, the dielectric constant E, and0denotes the air dielectric constant, t denotes time, P ═ Sigmai＝a,bPiRepresenting the electrical polarization density of the gain material.
As shown in FIG. 8, PaIs a second energy level N2And a first energy level N1The induced polarization density of atomic transitions between. PbAt a third energy level N3And the ground state energy level N0The induced polarization density of atomic transitions between. The electrons being from the ground level N0To a third energy level N3At pumping frequency omegabPumping, wherein the pumping frequency
E3Is the energy level represented by the third energy level, E0The magnitude of the energy represented by the ground state energy level,
is Planck constant. Second energy level N2Is the upper energy level of a metastable laser. Over a short time t32After that, the particles are at a third energy level N3Upper is rapidly transferred to the second energy level N by non-radiative transition2Second energy level N2Being metastable, having a longer lifetime, the particle may be at a second energy level N2Upper accumulation to realize three electric energy levels N3And a firstTwo energy level N2Population inversion of (2). When electrons radiate from high to low, they are at a central frequency ωaThe photons of the radiation are, among other things,
E2: the magnitude of the energy represented by the second energy level, E1: the magnitude of the represented energy of the first energy level,is Planck constant. Finally, the electron goes from the first energy level N1Upper rapid radiationless transfer to ground level N0. The atomic population density follows the following rate equation:
wherein, tau32Denotes the particles from N3Decline to N2Time of (d), τ21Denotes the particles from N2Decline to N1Time of (d), τ10Denotes the particles from N1Decline to N0Time of (d).
In optically pumping electrons from the ground level N0 to the third level N3 without using external electromagnetic waves, equations (2) and (5) can be obtained by pumping at a uniform pumping speed fpumpPumping electrons to simplify and uniform pumping speed fpumpProportional to the optical pumping intensity in the experiment. Based on this simplification, the following equation is derived:
the embodiment of the invention also provides a parameter determination method of the silicon cylindrical particles applied to the laser emitter, which comprises the following steps:
determining the diameter of the silicon cylindrical particles according to the working wavelength of the laser; preferably, the working wavelength of the laser is 1500 nm; electric resonance is a basis for laser emitters capable of generating laser light, and the prior art has been disclosedGenerating electric resonance, wherein lambda is the working wavelength, and D is the diameter of a silicon cylindrical particle; in the embodiment of the present application, the silicon cylindrical particles of the reflector are periodically arranged, when the silicon cylindrical particles are periodically arranged, the obtained reflector resonates at a wavelength higher than that of a single silicon cylinder, and experimental simulation shows that when the diameter of the silicon cylindrical particles of the reflector is 400nm, electrical resonance is generated.
The aspect ratio at which the reflectance is the preset reflectance is determined through experiments.
Determining the thickness of the silicon cylindrical particle of the mirror according to the aspect ratio and the diameter of the silicon cylindrical particle, comprising: using the formula of diameter to aspect ratioCalculating to obtain the thickness of the silicon cylindrical particle, wherein αiAspect ratio of silicon cylindrical particles, S, as a mirroriThickness of silicon cylindrical particle as mirror, DiThe diameter of the silicon cylinder particle is 1 or 2, and when 1, the mirror is the first mirror 1, and when 2, the mirror is the second mirror 2.
A graph of the relationship between the reflectivity of the mirror and the period of the silicon cylindrical particle arrangement and a line graph of the relationship between the modulation bandwidth of the mirror and the period of the silicon cylindrical particle arrangement are obtained through experiments.
Determining the periodic range of the silicon cylindrical particle arrangement when the reflectivity of the reflector is a preset reflectivity according to a relation curve graph of the reflectivity of the reflector and the period of the silicon cylindrical particle arrangement; when the reflectivity of the reflector is close to 1, the period range is 630-660 nm.
Determining the period of the silicon cylindrical particle arrangement when the reflectivity of the reflector is the preset reflectivity according to a relation line graph of the modulation bandwidth of the reflector and the period of the silicon cylindrical particle arrangement; when the period is 630nm, the bandwidth is much larger than the other bandwidths, and therefore, the period width is selected to be 630 nm.
By utilizing the parameter determination method of the silicon cylindrical particles applied to the laser emitter, provided by the embodiment of the invention, the thickness of the silicon cylindrical particles of the first reflector 1 is determined to be 460nm, the diameter is determined to be 400nm, and the period is determined to be 630 nm; the thickness of the silicon cylindrical particles of the second reflector 2 is 465nm, the diameter is 400nm, and the period is 630 nm; preferably, the operating wavelength is 1500nm, and each of the first mirror 1 and the second mirror 2 is composed of 16 periodically arranged silicon cylindrical particles.
The quality factor is an important indicator of laser light. In order to obtain a laser with a higher quality factor, the reflectivity between the two mirrors should be as close as possible. For the laser cavity, the quality factor is:
wherein Q is a quality factor v0Is the mode frequency, n0Is the refractive index of the medium in the cavity, c is the speed of light, d is the distance between the pillars, α is the aspect ratio of the silicon cylindrical particles, R1Is the reflectivity, R, of the first mirror 12Is the reflectivity of the second mirror 2.
The reflectance R of the first mirror 1 can be found by the formula (10)1The reflectivity R of the second mirror 2 can be almost 100%2The closer to 100%, the higher the quality factor Q, the better the quality of the laser. The reflectivity of the second reflector 2 can be less than 100% but more than 99% by slightly increasing the thickness of the silicon cylindrical particle, that is, the laser emitter provided by the embodiment of the present application achieves a method for controlling the reflectivity of the reflector by only slightly increasing the thickness of the silicon cylindrical particle, thereby showing good micro-control capability for the laser emitter. Compared with the traditional distributed Bragg reflector, the laser transmitter provided by the embodiment of the application is really easy to control, simple to prepare and convenient to produce.
The thickness of the reflector of the laser transmitter provided by the embodiment of the application is only 460nm, and when the reflectivity of the reflector of the distributed Bragg reflector reaches more than 99%, the size of the reflector of the distributed Bragg reflector is at least 1450 nm. When the reflectivity of the reflector of the distributed bragg reflector reaches more than 99% and the working wavelength is 1500nm, the quality factor Q is about 500, as shown in fig. 9; when the working wavelength of the laser transmitter provided by the embodiment of the application is 1500nm (the frequency is 200THz), the maximum quality factor Q is 2505 (as shown in FIG. 10); therefore, the laser transmitter provided by the embodiment of the application effectively reduces the whole volume of the laser, and simultaneously increases the Q value of the laser, so that the laser linewidth is smaller, and the laser transmitter has better single-mode output stability and higher single-mode output power.
A laser time domain diagram and a corresponding laser frequency domain diagram of a laser transmitter provided by an embodiment of the present invention are shown in fig. 11 and 12.
The principles and embodiments of the present invention have been described herein using specific examples, which are provided only to help understand the method and the core concept of the present invention; meanwhile, for a person skilled in the art, according to the idea of the present invention, the specific embodiments and the application range may be changed. In view of the above, the present disclosure should not be construed as limiting the invention.
Claims (10)
1. A laser transmitter based on all-dielectric super surface is characterized in that,
the laser emitter comprises the following components in sequence from bottom to top: a first mirror, an active layer, and a second mirror;
the first reflecting mirror and the second reflecting mirror are each composed of periodically arranged silicon cylindrical particles.
2. The all-dielectric super surface based laser transmitter according to claim 1, further comprising: a first confinement layer and a second confinement layer;
the first confinement layer is disposed between the first mirror and the active layer; the second confinement layer is disposed between the active layer and the first mirror; the first limiting layer and the second limiting layer are used for limiting carriers and adjusting resonance wavelength to enable the resonance wavelength to be equal to laser wavelength.
3. The all-dielectric super surface based laser transmitter according to claim 1, further comprising: a substrate;
the substrate is located below the first mirror.
4. The all-dielectric super surface based laser transmitter according to claim 1, further comprising: a first metal contact layer and a second metal contact layer;
the first metal contact layer is positioned below the substrate and is in ohmic contact with the substrate;
the second metal contact layer is located on the second mirror, and the second metal contact layer is in ohmic contact with the second mirror.
5. The all-dielectric-based super-surface laser emitter according to claim 1, wherein the silicon cylindrical particles of the first mirror are doped with trivalent elements; and pentavalent elements are doped into the silicon cylindrical particles of the second reflector.
6. The all-dielectric-based super-surface laser emitter according to claim 1, wherein a light outlet is formed on each of the second reflector and the second metal contact layer; the light outlet is used for outputting laser beams.
7. The all-dielectric-based super surface laser transmitter according to claim 6, wherein the active layer comprises a plurality of quantum well layers.
8. The all-dielectric-super-surface-based laser transmitter according to claim 7, wherein a plurality of the quantum well layers are filled with a gain medium.
9. A method for determining parameters of silicon cylindrical particles applied to the laser emitter of any one of claims 1 to 8, wherein the method for determining parameters comprises:
determining the diameter of silicon cylindrical particles of the reflector according to the working wavelength of the laser;
determining the aspect ratio of the silicon cylindrical particles when the reflectivity of the reflector is the preset reflectivity through an experiment;
determining the thickness of the silicon cylindrical particles of the reflector according to the aspect ratio and the diameter of the silicon cylindrical particles;
obtaining a relation curve diagram of the reflectivity of the reflecting mirror and the period of the silicon cylindrical particle arrangement and a relation curve diagram of the modulation bandwidth of the reflecting mirror and the period of the silicon cylindrical particle arrangement through experiments;
and determining the period of the silicon cylindrical particle arrangement when the reflectivity of the reflector is a preset reflectivity according to a relation line graph of the modulation bandwidth of the reflector and the period of the silicon cylindrical particle arrangement.
10. The method for determining the parameters of the silicon cylindrical particle of the all-dielectric-super-surface-based laser emitter according to claim 9, wherein the determining the thickness of the silicon cylindrical particle of the reflector according to the aspect ratio and the diameter of the silicon cylindrical particle comprises:
according to the aspect ratio and the diameter of the silicon cylindrical particles, using a formula
Calculating to obtain the thickness of the silicon cylindrical particles of the reflector;
wherein, αiAspect ratio of silicon cylindrical particles, S, as a mirroriThickness of silicon cylindrical particle as mirror, DiThe diameter of the silicon cylinder particle is 1 or 2, and when 1, the mirror is the first mirror, and when 2, the mirror is the second mirror.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201911075885.0A CN110797747B (en) | 2019-11-06 | 2019-11-06 | Laser transmitter based on all-dielectric super surface and parameter determination method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201911075885.0A CN110797747B (en) | 2019-11-06 | 2019-11-06 | Laser transmitter based on all-dielectric super surface and parameter determination method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN110797747A true CN110797747A (en) | 2020-02-14 |
| CN110797747B CN110797747B (en) | 2020-09-01 |
Family
ID=69443264
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201911075885.0A Active CN110797747B (en) | 2019-11-06 | 2019-11-06 | Laser transmitter based on all-dielectric super surface and parameter determination method |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN110797747B (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111817134A (en) * | 2020-09-03 | 2020-10-23 | 武汉云岭光电有限公司 | Vertical cavity surface emitting laser and manufacturing method thereof, coupling device and manufacturing method thereof |
| WO2023083110A1 (en) * | 2021-11-09 | 2023-05-19 | 深圳迈塔兰斯科技有限公司 | Superlens antireflection film design method and apparatus, electronic device |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103597676A (en) * | 2011-05-17 | 2014-02-19 | 丹麦技术大学 | Reflectivity-modulated grating mirror |
| US20170082842A1 (en) * | 2014-01-30 | 2017-03-23 | Shaltout Amr Mohammad E A | Ultra-small cavity with reflecting metasurfaces |
| CN108616033A (en) * | 2018-05-10 | 2018-10-02 | 中山大学 | Super surface is integrated in the orbital angular momentum ballistic device and preparation method thereof of VCSEL |
| CN108988123A (en) * | 2018-07-26 | 2018-12-11 | 华中科技大学 | Single-chip integration face emitting semiconductor laser and preparation method thereof based on super surface |
| CN109038214A (en) * | 2018-07-26 | 2018-12-18 | 华中科技大学 | Vertical cavity surface emitting laser and preparation method thereof based on super surface |
| CN109088307A (en) * | 2018-07-26 | 2018-12-25 | 华中科技大学 | Narrow line wide cavity laser based on super surface narrowband reflection mirror |
-
2019
- 2019-11-06 CN CN201911075885.0A patent/CN110797747B/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103597676A (en) * | 2011-05-17 | 2014-02-19 | 丹麦技术大学 | Reflectivity-modulated grating mirror |
| US20170082842A1 (en) * | 2014-01-30 | 2017-03-23 | Shaltout Amr Mohammad E A | Ultra-small cavity with reflecting metasurfaces |
| CN108616033A (en) * | 2018-05-10 | 2018-10-02 | 中山大学 | Super surface is integrated in the orbital angular momentum ballistic device and preparation method thereof of VCSEL |
| CN108988123A (en) * | 2018-07-26 | 2018-12-11 | 华中科技大学 | Single-chip integration face emitting semiconductor laser and preparation method thereof based on super surface |
| CN109038214A (en) * | 2018-07-26 | 2018-12-18 | 华中科技大学 | Vertical cavity surface emitting laser and preparation method thereof based on super surface |
| CN109088307A (en) * | 2018-07-26 | 2018-12-25 | 华中科技大学 | Narrow line wide cavity laser based on super surface narrowband reflection mirror |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN111817134A (en) * | 2020-09-03 | 2020-10-23 | 武汉云岭光电有限公司 | Vertical cavity surface emitting laser and manufacturing method thereof, coupling device and manufacturing method thereof |
| WO2023083110A1 (en) * | 2021-11-09 | 2023-05-19 | 深圳迈塔兰斯科技有限公司 | Superlens antireflection film design method and apparatus, electronic device |
Also Published As
| Publication number | Publication date |
|---|---|
| CN110797747B (en) | 2020-09-01 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| WO2021109350A1 (en) | Energy band inversion and optical field confinement effect-based topological bulk laser and method | |
| CN106058642B (en) | The narrow spectral line width surface-emitting laser of high contrast grating coupler | |
| CN110797747B (en) | Laser transmitter based on all-dielectric super surface and parameter determination method | |
| JP2003504880A (en) | Polarization control of vertical cavity surface emitting laser | |
| Song et al. | Subwavelength hybrid plasmonic nanodisk with high Q factor and Purcell factor | |
| Shang et al. | Advanced lanthanide doped upconversion nanomaterials for lasing emission | |
| CN103066495B (en) | Plasma nano laser device | |
| Reddy et al. | Analysis of lasing in dye-doped photonic crystals | |
| Peng et al. | ZIM laser: Zero-index-materials laser | |
| CN1710763A (en) | Optical pump high-power vertical external cavity emitting laser | |
| Xu et al. | Compact vertical-cavity surface-emitting laser based on all-dielectric metasurfaces | |
| Wang et al. | Controllable lasing behavior enabled by the transmission guided-mode resonance effect in coupled gratings | |
| Stockman | Spaser, plasmonic amplification, and loss compensation | |
| Viktorovitch et al. | Surface addressable photonic crystal membrane resonators: generic enablers for 3D harnessing of light | |
| CN111934196A (en) | Electrically-driven on-chip integrated erbium-doped waveguide amplifier and preparation method thereof | |
| WO2015080666A1 (en) | Light source including a nanoparticle | |
| Kumar et al. | Widely tunable mirror based on 3D hollow waveguide for tunable photonic integrated circuits | |
| Liu et al. | Unidirectional transmission in finite-size high-contrast gratings | |
| Dong et al. | The giant enhancement of Fano-type resonance in a gain-assisted silicon slab array | |
| CN118151276B (en) | Optical microcavity and optical device | |
| Hong et al. | Ultrahigh quality factor cavity based on double dielectric nanocylinder metasurfaces | |
| Zhang et al. | Boundary rounding effect in the hexagonal and oval two-dimensional optical microcavity | |
| Lu et al. | Topological Laser in Anomalous Quadrupole Topological Phases | |
| Chen et al. | Planar plasmonic lens based on circular nanohole in a gold film in visible light range | |
| Cui et al. | Design of a four-energy-level vertical external surface-emission laser enabled on the waveguide grating structure |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |