CN109613635B - Novel ultra-narrow band wave absorber with metal nano ring column array structure - Google Patents

Novel ultra-narrow band wave absorber with metal nano ring column array structure Download PDF

Info

Publication number
CN109613635B
CN109613635B CN201910035610.8A CN201910035610A CN109613635B CN 109613635 B CN109613635 B CN 109613635B CN 201910035610 A CN201910035610 A CN 201910035610A CN 109613635 B CN109613635 B CN 109613635B
Authority
CN
China
Prior art keywords
ring column
nano ring
narrow band
absorber
nano
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.)
Active
Application number
CN201910035610.8A
Other languages
Chinese (zh)
Other versions
CN109613635A (en
Inventor
伍铁生
王学玉
张慧仙
王宜颖
曹卫平
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Guilin University of Electronic Technology
Original Assignee
Guilin University of Electronic Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Guilin University of Electronic Technology filed Critical Guilin University of Electronic Technology
Priority to CN201910035610.8A priority Critical patent/CN109613635B/en
Publication of CN109613635A publication Critical patent/CN109613635A/en
Application granted granted Critical
Publication of CN109613635B publication Critical patent/CN109613635B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/003Light absorbing elements
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/008Surface plasmon devices

Landscapes

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

Abstract

The invention relates to a novel ultra-narrow band absorber of a metal nano ring column array structure, which solves the technical problem of poor quality factor, and the ultra-narrow band absorber based on surface lattice resonance is composed of a nano ring column array; the nano array unit is sequentially arranged into a dielectric layer substrate, a metal film reflecting layer and a resonator from bottom to top; the thickness of the thin film gold of the reflecting layer of the nano array unit is larger than the skin depth of the incident electromagnetic wave in noble metal gold; the nano array unit adopts a double-ring column structure to compress the full width half maximum of the absorption spectrum of the wave absorber, so that the problems of low absorption efficiency, large full width half maximum, low quality factor and the like of the traditional wave absorber are well solved, and the nano array unit can be used in the application of a narrow-band heat radiator and a plasma biosensor.

Description

Novel ultra-narrow band wave absorber with metal nano ring column array structure
Technical Field
The invention relates to the field of ultra-narrow band wave absorbers, in particular to a novel ultra-narrow band wave absorber with a metal nano ring column array structure.
Background
In recent years, narrowband absorbers based on surface lattice resonance have been attracting attention in many fields. The ultra-narrow band absorber with nanometer scale has the characteristics of small volume, high sensitivity, wide market application prospect, easy mass production and the like, and is more and more paid attention to. The conventional structure of the traditional narrow-band absorber is a metal-medium-metal structure, but the generated surface lattice resonance effect is less obvious, the quality factor of the absorber is obviously reduced, and the application of the narrow-band absorber is limited.
In order to solve the technical problem of small quality factor of the existing ultra-narrow band absorber, the invention provides an ultra-narrow band absorber based on surface lattice resonance of a nano-structure metal surface, which can generate strong surface lattice resonance effect and ultra-high optical interaction at resonance absorption wavelength to obtain a higher quality factor. The ultra-narrow band wave absorber based on surface lattice resonance has a great application and development prospect in the aspects of a narrow band heat radiator, a high-sensitivity biosensor and the like.
Disclosure of Invention
The invention provides a novel ultra-narrow band absorber based on a metal nano ring column array structure, which has the characteristic of higher quality factor.
In order to improve the quality factor of the narrow-band absorber, the following technical scheme is adopted:
the novel ultra-narrow band wave absorber of the metal nano ring column array structure comprises nano structure units which are periodically arranged; the nanostructure unit is sequentially provided with a medium substrate, a bottom continuous metal film and a resonator from bottom to top; the thickness of the bottom continuous metal film is larger than the skin depth of the incident wave on the bottom continuous metal film layer;
the resonator comprises two concentric metal nano ring columns; the first concentric metal nano ring column is positioned below the second concentric metal nano ring column, the inner diameters of the two nano ring columns are equal, the outer diameter of the first nano ring column is larger than that of the second nano ring column, and the heights of the first nano ring column and the second nano ring column are equal; the first nano ring column and the second nano ring column are connected in a seamless manner;
the vertical cross sections of the medium substrate and the bottom continuous metal film are rectangular; the horizontal cross sections of the dielectric substrate and the bottom continuous metal film are square and have the same size.
The working principle of the invention is as follows: because the wave absorbing component of the designed ultra-narrow band wave absorber is composed of the same metal, the periodic nano structure can generate stronger surface lattice resonance, and meanwhile, stronger optical coupling effect is generated between the resonator and the gold film, so that the device can obtain higher quality factor. Surface lattice resonances are essentially complex localized surface plasmon resonances that have not only periodic effects on the diffraction orders of the periodic array, but are also affected by the plasmonic nature of the metal structure. Whereas for our designed structure the resonant wavelength increases linearly with period. The narrowband absorber structure has a smaller periodicity due to the stronger coupling effect and stronger surface lattice resonance effect of each structural unit. Also, we can reduce the coupling between the structural units by increasing the size of the period and thus the resonance bandwidth.
The nanostructure is made of gold and the highly reflective underlayer below the designed nanostructure provides strong optical interactions and scatters light back into the air rather than down into the dielectric, compared to conventional metal-dielectric-metal structures. By eliminating this forward scattering, the radiation loss is significantly reduced, contributing to a narrower absorption band. The all-metal absorber drives electromagnetic field resonance from the substrate interface to the top surface of the nanostructure. The excitation mode from the top surface may be more than three times higher in local field strength than the metal-dielectric-metal structure. In general, highly excited surface lattice resonances excited by the underlying metal substrate can provide a sharper absorption spectrum and a higher quality factor.
In the above scheme, for optimization, further, the material of the bottom continuous metal film is gold.
Further, the length and the width of the bottom continuous metal film are p=1000 nm, and the thickness h=200 nm; the inner diameter d1=100 nm, the outer diameter d3=300 nm and the height h2=40 nm of the first metal nano ring column; the inner diameter d1=100 nm, the outer diameter d2=210 nm and the height h1=40 nm of the second metal nano ring column.
Further, the working wavelength range of the novel ultra-narrow band absorber is 700-1800nm.
The invention has the beneficial effects that: the nanometer ultra-narrow band absorber is of a periodic structure, is simple in structure, compact in structure, perfectly symmetrical and easy to realize; the invention provides a nanometer ultra-narrow band absorber, and the resonance wavelength modulation range is 900nm to 1500nm. The absorption of resonance wavelengths in the period from 600nm to 1000nm exceeds 70%, the quality factor is as high as 80, and the refractive index sensitivity is as high as 1020nm/RIU, particularly, it should be pointed out that the previously reported narrow-band absorbers have difficulty in achieving such high quality factors.
Drawings
The invention will be further described with reference to the drawings and examples.
Fig. 1 is a three-dimensional schematic diagram of the wave absorber array unit.
Fig. 2 shows the absorption rate of the absorber according to example 1 as a function of wavelength and period in air.
Fig. 3 shows the trend of the light absorptivity of the absorber described in example 1 with wavelength and period.
Fig. 4, application of the absorber described in example 1 in the sensor field.
Fig. 5 shows that the refractive index sensitivity of the absorber described in example 1 as a micro-nano sensor increases with the period of the structure.
FIG. 6 shows a wavelength absorber of the embodiment 1 as a micro-nano photothermal radiometer with a period of 1000nm, an ambient refractive index of 1 (air environment), an ambient temperature of 300K, an excitation wavelength of resonance wavelength, and an incident light intensity of 100mW/cm 2 From the temperature profile obtained by the simulation, the device temperature increased by 5.6K at thermal steady state.
FIG. 7 shows a wavelength absorber of the embodiment 1 as a micro-nano photothermal radiometer, the period being 1000nm, the ambient refractive index being 1 (air environment), the ambient temperature being 300K, the excitation wavelength being the resonance wavelength, the incident light intensity being 100mW/cm 2 The relationship between the input light intensity and the temperature increase of the absorber at thermal steady state.
Detailed Description
The present invention will be described in further detail with reference to the following examples in order to make the objects, technical solutions and advantages of the present invention more apparent. It should be noted that the specific embodiments described herein are for the purpose of illustrating the invention only and are not to be construed as limiting the invention.
Example 1
The embodiment provides a novel ultra-narrow band absorber of a metal nano ring column array structure, which consists of a periodic metal nano ring column structure; the nano ring column array structure sequentially comprises a medium substrate, a bottom continuous metal film layer and a resonator from bottom to top; the nano ring column is of a double-ring column structure with the same wall thickness of the ring column; the thickness of the bottom continuous metal film layer is larger than the skin depth of incident waves in the same material metal of the bottom continuous metal film layer.
As shown in fig. 1, the bottom of the nano ring column array structure is a cuboid made of gold material, a first nano ring column is arranged on the cuboid, the first nano ring column is positioned below a second nano ring column, the inner diameters of the two nano ring columns are equal, and the first nano ring column and the second nano ring column are directly overlapped; the first nano ring column and the second nano ring column are made of gold. The length and width p=1000 nm of the bottom metal and the thickness h=200 nm; the inner diameter d1=100 nm, the outer diameter d3=300 nm and the height h2=40 nm of the first nano ring column; the second nanoring column has an inner diameter d1=100 nm, an outer diameter d2=210 nm, and a height h1=40 nm.
Simulation calculations were performed using FDTD solutions software, as in fig. 2. It can be seen that in the wavelength range 700nm-1800nm the resonance frequency gradually red shifts from 900nm to 1500nm. When the background refractive index is 1 and the period is 600nm-1000nm, the absorption peak value is over 70%. The refractive index sensitivity increases gradually from 675nm/RIU to 1020nm/RIU as the period changes from 600nm to 1100 nm. This demonstrates that the metamaterial-structured ultra-narrow-band absorber designed in this embodiment has significant advantages both in terms of structure and index parameters.
As shown in fig. 1, the ultra-narrow band absorber of the present embodiment is simple and compact in structure. The dielectric substrate of this embodiment may be a conventional silicon dioxide substrate material, or may be another dielectric material, which does not act on the surface lattice resonance of the device as a substrate. The optimized ultra-narrow band absorber bottom continuous metal film layer and the nano ring column are all made of gold, and the material is single and easy to realize.
As shown in fig. 2, the absorption spectra of the ultra-narrow band absorber of the present embodiment under different periodic conditions are given. Simulation shows that the period of the nano array is in the range of 600nm to 1000nm, and the highest peak absorption of the absorber is more than 70%. And as the period increases, the resonance absorption wavelength undergoes a red shift phenomenon.
As shown in fig. 3, the trend of the change in light absorption efficiency with wavelength and period of the ultra-narrow band absorber of the present embodiment is given. The wavelength range is 700nm-1700nm, when the period change range is 600 nm-800 nm, the absorption spectrum has only one peak absorption, but the full width at half maximum of the peak is too large, so that the quality factor is reduced; when the period variation ranges between 800nm and 1200nm, the absorption spectrum exhibits two absorption peaks. The absorption peak corresponding to longer wavelength has high absorption rate and narrow half-width. The absorption peak mentioned in this patent refers to an absorption peak corresponding to a longer wavelength unless otherwise specified.
As shown in fig. 4, the application of the ultra-narrow band absorber of the present embodiment in the field of refractive index sensing is illustrated. The period of the ultra-narrow band absorber is set to be 1000nm, the refractive index of the analysis liquid is increased from 1.30 to 1.50, the resonance absorption peak value of the analysis liquid is also more than 90%, and the resonance wavelength is linearly increased along with the increase of the refractive index; at refractive indices of the analytes of 1.30 and 1.50, the resonance wavelengths were 1350nm and 1550nm, respectively.
As shown in fig. 5, the effect of the period of the ultra-narrow band absorber of the present embodiment on the refractive index sensitivity is demonstrated. It can be seen that the refractive index sensitivity increases gradually from 675nm/RIU to 1020nm/RIU as the period changes from 600nm to 1100 nm. From this, it is understood that the refractive index sensing sensitivity of the ultra-narrow band absorber of the present embodiment can be adjusted by the period.
As shown in fig. 6, the application of the ultra-narrow band absorber of the present embodiment in the field of heat radiators is illustrated. The period is 1000nm, the ambient refractive index is 1 (air environment), the ambient temperature is 300K, the excitation wavelength is the resonance wavelength, and the incident light intensity is 100W/cm 2 From the temperature profile obtained by the simulation, the device temperature increased by 5.6K at thermal steady state. Simulation results show that the ultra-narrow band absorber has remarkable photo-thermal conversion efficiency and can be used as a micro-nano heat radiator.
As shown in fig. 7, the absorber described in example 1 shows the relationship between the increase in the photothermal conversion temperature of the ultra-narrow band absorber and the intensity of incident light in this example as a micro-nano photothermal radiometer. The period is 1000nm, the ambient refractive index is 1 (air environment), the ambient temperature is 300K, the excitation wavelength is the resonance wavelength, and the incident light intensity is 100W/cm 2 It can be seen that at thermal steady state conditions, the temperature of the absorber increases linearly with increasing light intensity.
In this embodiment, the skin depth of the incident wave in the underlying continuous metal film does not exceed 100nm over the frequency range under consideration. Therefore, the bottom continuous metal film is set to 200nm to effectively prevent electromagnetic waves from transmitting through the absorber.
The working wavelength range of the novel ultra-narrow band absorber in the embodiment is 700nm-1800nm.
While the foregoing describes the illustrative embodiments of the present invention so that those skilled in the art may understand the present invention, the present invention is not limited to the specific embodiments, and all inventive innovations utilizing the inventive concepts are herein within the scope of the present invention as defined and defined by the appended claims, as long as the various changes are within the spirit and scope of the present invention.

Claims (2)

1. A novel ultra-narrow band wave absorber of a metal nano ring column array structure is characterized in that: the novel ultra-narrow band wave absorber of the metal nano ring column array structure consists of a periodic metal nano ring column structure; the nano ring column array structure sequentially comprises a medium substrate, a bottom continuous metal film layer and a resonator from bottom to top; the thickness of the bottom continuous metal film layer is larger than the skin depth of incident waves in the metal of the same material as the bottom continuous metal film layer;
the resonator comprises two concentric metal nano ring columns; the first concentric metal nano ring column is positioned below the second concentric metal nano ring column, the inner diameters of the two ring columns are equal, the outer diameter of the first nano ring column is larger than that of the second nano ring column, and the heights of the two ring columns are equal; the first nano ring column and the second nano ring column are directly overlapped without an intermediate medium layer;
the vertical cross sections of the medium substrate and the bottom continuous metal film are rectangular; the horizontal cross sections of the dielectric substrate and the bottom continuous metal film are square and have the same size;
the bottom continuous metal film is made of gold;
the length and the width of the bottom continuous metal film are p=1000 nm, and the height h=200 nm;
the inner diameter d1=100 nm, the outer diameter d3=300 nm and the height h2=40 nm of the first concentric metal nano ring column;
the inner diameter d1=100 nm, the outer diameter d2=210 nm and the height h1=40 nm of the second concentric metal nano ring column;
the dielectric substrate includes a silicon dioxide substrate material.
2. The novel ultra-narrow band absorber of the metal nano ring pillar array structure according to claim 1, wherein: the working wavelength range of the novel ultra-narrow band absorber of the metal nano ring column array structure is 700nm-1800nm.
CN201910035610.8A 2019-01-15 2019-01-15 Novel ultra-narrow band wave absorber with metal nano ring column array structure Active CN109613635B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910035610.8A CN109613635B (en) 2019-01-15 2019-01-15 Novel ultra-narrow band wave absorber with metal nano ring column array structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910035610.8A CN109613635B (en) 2019-01-15 2019-01-15 Novel ultra-narrow band wave absorber with metal nano ring column array structure

Publications (2)

Publication Number Publication Date
CN109613635A CN109613635A (en) 2019-04-12
CN109613635B true CN109613635B (en) 2024-04-02

Family

ID=66017321

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910035610.8A Active CN109613635B (en) 2019-01-15 2019-01-15 Novel ultra-narrow band wave absorber with metal nano ring column array structure

Country Status (1)

Country Link
CN (1) CN109613635B (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110196464B (en) * 2019-07-01 2022-07-29 江南大学 Method for realizing ultra-wideband light absorption and composite microstructure
CN110749946B (en) * 2019-12-06 2021-12-03 陕西师范大学 Metal-medium-metal based enhanced absorption structures, devices and systems
CN111308587B (en) * 2020-03-02 2022-06-28 江西师范大学 Tunable multi-band ultra-narrow band electromagnetic wave absorber
CN111580197B (en) * 2020-05-17 2022-05-17 桂林电子科技大学 Transverse MIMI lattice plasmon resonance absorber
CN112114391B (en) * 2020-10-21 2021-12-28 电子科技大学 Plasmon absorber and preparation method thereof
CN112558200B (en) * 2020-12-04 2023-04-07 中国人民解放军国防科技大学 Metamaterial wave absorber and manufacturing method thereof
CN112882144B (en) * 2021-01-21 2021-11-30 北京理工大学 Ultraviolet filtering structure based on nanoring patterned interface and design method thereof
CN113075755A (en) * 2021-03-25 2021-07-06 桂林电子科技大学 Light trapping structure based on LSPR effect and preparation method thereof
CN113387318B (en) * 2021-06-11 2024-02-09 中国科学技术大学 Near-infrared band-pass filter based on nano annular array and preparation method thereof
CN114280710B (en) * 2021-12-19 2024-02-02 复旦大学 Super-structured surface with bicontinuous spectrum binding state characteristics

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20010076749A (en) * 2000-01-27 2001-08-16 다까하시 미찌하루 Wide-band ferrite electromagnetic wave absorber
KR20150000616A (en) * 2013-06-25 2015-01-05 한국과학기술연구원 Broadbadn visible light absorption nanostructure using plasmon
JP2016020887A (en) * 2014-06-17 2016-02-04 シャープ株式会社 Sensing element and sensing method
CN105652354A (en) * 2016-01-25 2016-06-08 中国科学院上海光学精密机械研究所 Polarization-independent broadband absorber based on conical metal-dielectric multilayer grating structure
CN105720378A (en) * 2016-01-13 2016-06-29 武汉科技大学 Polarization-insensitive photic driving tunable TeraHertz wave metamaterial absorber
CN107994348A (en) * 2017-11-28 2018-05-04 中国计量大学 The double off-centre operation THz wave absorbers of non-same layer
CN108336505A (en) * 2018-01-31 2018-07-27 电子科技大学 A kind of insensitive Meta Materials of terahertz wave band broadband polarization
CN209198690U (en) * 2019-01-15 2019-08-02 桂林电子科技大学 A kind of novel ultra-narrow band wave absorbing device of metal nano annulated column array structure

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB201112740D0 (en) * 2011-07-25 2011-09-07 Qinetiq Ltd Radiation absorption

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20010076749A (en) * 2000-01-27 2001-08-16 다까하시 미찌하루 Wide-band ferrite electromagnetic wave absorber
KR20150000616A (en) * 2013-06-25 2015-01-05 한국과학기술연구원 Broadbadn visible light absorption nanostructure using plasmon
JP2016020887A (en) * 2014-06-17 2016-02-04 シャープ株式会社 Sensing element and sensing method
CN105720378A (en) * 2016-01-13 2016-06-29 武汉科技大学 Polarization-insensitive photic driving tunable TeraHertz wave metamaterial absorber
CN105652354A (en) * 2016-01-25 2016-06-08 中国科学院上海光学精密机械研究所 Polarization-independent broadband absorber based on conical metal-dielectric multilayer grating structure
CN107994348A (en) * 2017-11-28 2018-05-04 中国计量大学 The double off-centre operation THz wave absorbers of non-same layer
CN108336505A (en) * 2018-01-31 2018-07-27 电子科技大学 A kind of insensitive Meta Materials of terahertz wave band broadband polarization
CN209198690U (en) * 2019-01-15 2019-08-02 桂林电子科技大学 A kind of novel ultra-narrow band wave absorbing device of metal nano annulated column array structure

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
基于局域表面等离子体共振吸波体的设计与仿真;王学玉;《中国优秀硕士论文电子期刊网》;20200531;第13页-20页 *
基于超材料结构的电磁波吸收特性研究;雷建国;《中国博士学位论文全文数据库》;第14-16、42-61页 *

Also Published As

Publication number Publication date
CN109613635A (en) 2019-04-12

Similar Documents

Publication Publication Date Title
CN109613635B (en) Novel ultra-narrow band wave absorber with metal nano ring column array structure
Yi et al. Broadband polarization-insensitive and wide-angle solar energy absorber based on tungsten ring-disc array
Jiang et al. Multi-band and high-sensitivity perfect absorber based on monolayer graphene metamaterial
Wang et al. A novel plasmonic refractive index sensor based on gold/silicon complementary grating structure
Tian et al. All-solid D-shaped photonic fiber sensor based on surface plasmon resonance
CN209198690U (en) A kind of novel ultra-narrow band wave absorbing device of metal nano annulated column array structure
Hao et al. Nearly total absorption of light and heat generation by plasmonic metamaterials
Liu et al. A square-lattice D-shaped photonic crystal fiber sensor based on SPR to detect analytes with large refractive indexes
Pan et al. A narrowband perfect absorber with high Q-factor and its application in sensing in the visible region
CN108519352B (en) Refractive index sensor based on metal-medium-metal waveguide Bragg grating
CN109030415B (en) Refractive index sensor based on double Fano resonance
CN110530820B (en) Dual-waveband plasmon sensor based on gold nano-antenna/graphene structure
CN111338011B (en) Method for realizing ultra-wideband light absorption enhancement by adopting composite microstructure
Zhang et al. All-dielectric refractive index sensor based on Fano resonance with high sensitivity in the mid-infrared region
CN111504947A (en) Surface plasmon refractive index sensor based on MIM annular grid point array
CN110146468B (en) Surface plasma optical fiber sensor with circular composite hole array structure
CN111122517A (en) Sensor based on asymmetric nanoparticle dimer micro-nano structure
Zhou et al. Cross-shaped titanium resonators based metasurface for ultra-broadband solar absorption
CN111879728A (en) Structure for improving quality factor of refractive index sensing device and testing method
CN111948175B (en) High-Q high-FoM metal medium auxiliary GMR refractive index sensing chip
CN112945905B (en) SPR-based high-sensitivity photonic quasicrystal fiber methane sensor
Ying et al. A review of recent research progress on optimization in D-shaped photonic crystal fiber
CN103926707B (en) Excitation and regulation method for waveguide resonance coupling surface plasma optical field
Xiangxian et al. Research on surface plasmon refractive index sensing of gold nano cone array and gold film coupling structure
Feng et al. Gold nano-double-ring array sensor based on Fano resonance

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