CN103457009A - Terahertz low-loss bent waveguide - Google Patents
Terahertz low-loss bent waveguide Download PDFInfo
- Publication number
- CN103457009A CN103457009A CN2013103609089A CN201310360908A CN103457009A CN 103457009 A CN103457009 A CN 103457009A CN 2013103609089 A CN2013103609089 A CN 2013103609089A CN 201310360908 A CN201310360908 A CN 201310360908A CN 103457009 A CN103457009 A CN 103457009A
- Authority
- CN
- China
- Prior art keywords
- waveguide plate
- waveguide
- plate
- terahertz
- loss
- 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
Landscapes
- Aerials With Secondary Devices (AREA)
- Optical Integrated Circuits (AREA)
Abstract
本发明涉及一种太赫兹低损耗弯曲波导,其包括外侧波导板和内侧波导板,外侧波导板和内侧波导板均为弯曲的金属板并且弯曲部为圆弧状,外侧波导板和内侧波导板彼此相距地平行布置,在外侧波导板和内侧波导板的彼此相对的表面上分别设有周期性凹槽。太赫兹波以横磁波模式从外侧波导板和内侧波导板的一端输入,进入外侧波导板和内侧波导板之间的间隙后形成表面波在该间隙中传输,进而传送到外侧波导板和内侧波导板的另一端,从而实现了太赫兹波的低损耗弯曲传输。根据本发明的技术方案,不仅太赫兹波弯曲损耗低,而且结构简单、使用方便、成本低廉。
The invention relates to a terahertz low-loss curved waveguide, which includes an outer waveguide plate and an inner waveguide plate, both of which are curved metal plates with arc-shaped curved parts, and the outer waveguide plate and the inner waveguide plate They are arranged in parallel with a distance from each other, and periodic grooves are respectively provided on the opposite surfaces of the outer waveguide plate and the inner waveguide plate. The terahertz wave is input from one end of the outer waveguide plate and the inner waveguide plate in the transverse magnetic wave mode, enters the gap between the outer waveguide plate and the inner waveguide plate, forms a surface wave and transmits in the gap, and then transmits to the outer waveguide plate and the inner waveguide The other end of the plate, thus realizing the low-loss bending transmission of terahertz waves. According to the technical solution of the present invention, not only the bending loss of the terahertz wave is low, but also the structure is simple, the use is convenient, and the cost is low.
Description
技术领域technical field
本发明涉及一种太赫兹低损耗弯曲波导。The invention relates to a terahertz low-loss curved waveguide.
背景技术Background technique
太赫兹(THz)波是位于微波和远红外线之间的电磁波。近年来,随着超快激光技术的发展,使得太赫兹脉冲的产生有了稳定、可靠的激发光源,使人们能够研究太赫兹。太赫兹在生物医学、安全监测、无损伤探测、天文学、光谱与成像技术以及信息科学等领域有着广泛的应用。太赫兹波导是太赫兹应用的一种基本的传输器件并且是太赫兹通信系统的关键器件。国际上,Maier等人于2008年研究了太赫兹波在结构化金属表面的传播特性(Nature Photonics,2,175-179,2008),Nahata等于2011年研究了矩形凹槽阵列上的伪表面等离子波导(Optics Express,19,1072-1080,2011),但是所有这些结构的横向电尺寸较大,导致在弯曲的情况下损耗较大。Terahertz (THz) waves are electromagnetic waves that lie between microwaves and far infrared rays. In recent years, with the development of ultrafast laser technology, the generation of terahertz pulses has a stable and reliable excitation light source, enabling people to study terahertz. Terahertz has a wide range of applications in biomedicine, safety monitoring, non-destructive detection, astronomy, spectroscopy and imaging technology, and information science. Terahertz waveguide is a basic transmission device for terahertz applications and a key device for terahertz communication systems. Internationally, Maier et al. studied the propagation characteristics of terahertz waves on structured metal surfaces in 2008 (Nature Photonics, 2, 175-179, 2008), and Nahata et al. studied pseudo-surface plasmon waveguides on rectangular groove arrays in 2011 ( Optics Express, 19, 1072-1080, 2011), but the lateral electrical dimensions of all these structures are large, resulting in large losses in the case of bending.
发明内容Contents of the invention
本发明的目的在于克服上述现有的波导在弯曲的情况下损耗较大的缺陷。The purpose of the present invention is to overcome the defect that the above-mentioned existing waveguide has relatively large loss in the case of bending.
为了实现这一目的,本发明提供了一种太赫兹低损耗弯曲波导,其包括外侧波导板和内侧波导板,外侧波导板和内侧波导板均为弯曲的金属板并且弯曲部为圆弧状,外侧波导板和内侧波导板彼此相距地平行布置,在外侧波导板和内侧波导板的彼此相对的表面上分别设有周期性凹槽。In order to achieve this purpose, the present invention provides a terahertz low-loss curved waveguide, which includes an outer waveguide plate and an inner waveguide plate, both of which are curved metal plates and the curved portion is arc-shaped, The outer waveguide plate and the inner waveguide plate are arranged in parallel with a distance from each other, and periodic grooves are respectively provided on the opposite surfaces of the outer waveguide plate and the inner waveguide plate.
优选地,外侧波导板和内侧波导板的金属材质为铝、铜、银、铁、镍中的一种。Preferably, the metal material of the outer waveguide plate and the inner waveguide plate is one of aluminum, copper, silver, iron, and nickel.
根据本发明的一优选实施例中,波导的弯曲角度为直角,弯曲半径大于500μm。According to a preferred embodiment of the present invention, the bending angle of the waveguide is a right angle, and the bending radius is greater than 500 μm.
根据本发明的一优选实施例中,其中外侧波导板和内侧波导板形状类似,外侧波导板上的凹槽和内侧波导板上的凹槽的尺寸和间隔周期均相同。According to a preferred embodiment of the present invention, the outer waveguide plate and the inner waveguide plate are similar in shape, and the grooves on the outer waveguide plate and the grooves on the inner waveguide plate have the same size and interval.
根据本发明的一优选实施例中,外侧波导板上的凹槽和内侧波导板上的凹槽关于外侧波导板和内侧波导板之间的中心线对称。According to a preferred embodiment of the present invention, the grooves on the outer waveguide plate and the grooves on the inner waveguide plate are symmetrical about the center line between the outer waveguide plate and the inner waveguide plate.
根据本发明的一优选实施例中,凹槽的宽度为50~500μm,深度为50~500μm,长度为不低于500μm;其中凹槽的宽度优选为152μm,深度优选为274μm。According to a preferred embodiment of the present invention, the width of the groove is 50-500 μm, the depth is 50-500 μm, and the length is not less than 500 μm; the width of the groove is preferably 152 μm, and the depth is preferably 274 μm.
根据本发明的一优选实施例中,凹槽的周期性间隔优选为475μm。According to a preferred embodiment of the present invention, the periodic interval of the grooves is preferably 475 μm.
根据本发明的一优选实施例中,外侧波导板的弯曲部两个表面的圆弧半径分别为0.8mm和1.2mm,而内侧波导板的弯曲部两个表面的圆弧半径分别为0.2mm和0.6mm。According to a preferred embodiment of the present invention, the arc radii of the two surfaces of the curved portion of the outer waveguide plate are 0.8 mm and 1.2 mm respectively, while the arc radii of the two surfaces of the curved portion of the inner waveguide plate are 0.2 mm and 1.2 mm respectively. 0.6mm.
根据本发明的一优选实施例中,外侧波导板与内侧波导板之间的间距为0.1~0.5mm,板间及凹槽内媒质为空气。According to a preferred embodiment of the present invention, the distance between the outer waveguide plate and the inner waveguide plate is 0.1-0.5 mm, and the medium between the plates and in the groove is air.
与现有技术相比,根据本发明的技术方案,不仅降低了太赫兹波弯曲损耗,而且结构简单、使用方便、成本低廉。Compared with the prior art, according to the technical solution of the present invention, not only the bending loss of the terahertz wave is reduced, but also the structure is simple, the use is convenient, and the cost is low.
附图说明Description of drawings
图1以立体图示意性示出了根据本发明一优选实施例的太赫兹低损耗弯曲波导的结构;Figure 1 schematically shows the structure of a terahertz low-loss curved waveguide according to a preferred embodiment of the present invention in a perspective view;
图2以侧视图进一步示意性示出了根据本发明一优选实施例的太赫兹低损耗弯曲波导的结构。Fig. 2 further schematically shows the structure of a terahertz low-loss curved waveguide according to a preferred embodiment of the present invention in a side view.
具体实施方式Detailed ways
下面结合附图详细描述本发明的太赫兹低损耗弯曲波导。本领域技术人员应当理解,下面描述的实施例仅是对本发明的示例性说明,而非用于对其作出任何限制。The terahertz low-loss curved waveguide of the present invention will be described in detail below with reference to the accompanying drawings. Those skilled in the art should understand that the embodiments described below are only illustrative illustrations of the present invention, and are not intended to limit it in any way.
如图1所示,在根据本发明的一优选实施例中,太赫兹低损耗弯曲波导包括两个金属板即外侧波导板1和内侧波导板2,这两个金属板均是弯曲的金属板,弯曲部(拐角处)为圆弧状,外侧波导板1和内侧波导板2平行放置并且外侧波导板1和内侧波导板2之间有一定的间隙,在外侧波导板1和内侧波导板2的相对的表面上设有周期性凹槽,也就是在外侧波导板1的内表面上设有周期性凹槽11以及在内侧波导板2的外表面上设有周期性凹槽21。另外,可以理解的是,凹槽的数量可根据实际所需的传输长度来确定,这里的传输长度指的是实际应用中太赫兹信号的传输长度,也就是波导的长度。As shown in Figure 1, in a preferred embodiment according to the present invention, the terahertz low-loss curved waveguide includes two metal plates, namely the
其中,外侧波导板1和内侧波导板2的形状可相类似,外侧波导板1上的凹槽11和内侧波导板2上的凹槽21的尺寸和间隔周期可均相同。优选地,凹槽11和凹槽21关于外侧波导板1和内侧波导板2之间的中心线呈对称状态分布。The
太赫兹波以横磁波模式从外侧波导板1和内侧波导板2的一端输入,进入外侧波导板1和内侧波导板2之间的间隙后形成表面波在该间隙中传输,进而传送到外侧波导板1和内侧波导板2的另一端,从而实现太赫兹波的低弯曲损耗传输。The terahertz wave is input from one end of the
需要指出的是,弯曲的金属板(也就是外侧波导板1和内侧波导板2)的弯曲角度可以为任意角度,例如90°。It should be pointed out that the bending angle of the bent metal plate (that is, the
波导的弯曲半径优选大于500μm,这里,波导的弯曲半径指的是外侧波导板1和内侧波导板2之间的中心线在弯曲部分的弯曲半径。The bending radius of the waveguide is preferably greater than 500 μm. Here, the bending radius of the waveguide refers to the bending radius of the center line between the
这种太赫兹弯曲波导可以低损耗地改变太赫兹波的传输方向。另外,本领域技术人员可以理解的是,可以通过调整凹槽尺寸以及外侧波导板1和内侧波导板2之间的板间距来实现不同波段的太赫兹波的传输。This terahertz curved waveguide can change the transmission direction of terahertz waves with low loss. In addition, those skilled in the art can understand that the transmission of terahertz waves in different wavebands can be realized by adjusting the groove size and the plate spacing between the
下面,参照图2进一步描述根据本发明一优选实施例的太赫兹低损耗弯曲波导的结构。如图2所示,外侧波导板1和内侧波导板2之间的距离D为200μm,凹槽11、21深度H为274μm,凹槽11、21宽度W为152μm,凹槽11、21出现的周期T为475μm,板长L1为3mm,板长L2为3mm,板厚S为0.4mm,板宽为2mm,圆弧半径R1为0.2mm,圆弧半径R2为0.6mm,圆弧半径R3为0.8mm,圆弧半径R4为1.2mm,该波导的弯曲半径为700μm,凹槽的长度与波导板宽度相同,外侧波导板1和内侧波导板2弯曲角度为90°,板间及凹槽内媒质为空气。Next, the structure of the terahertz low-loss curved waveguide according to a preferred embodiment of the present invention will be further described with reference to FIG. 2 . As shown in Figure 2, the distance D between the
接着,一并描述根据本发明一优选实施例的太赫兹低损耗弯曲波导的示例性主要加工步骤(下面的步骤1-2)及损耗测试(下面的步骤3-4)。Next, exemplary main processing steps (steps 1-2 below) and loss testing (steps 3-4 below) of the terahertz low-loss curved waveguide according to a preferred embodiment of the present invention are described together.
1)先用机械加工的方法按尺寸加工出一定厚度并且90°弯曲的金属板两块(外侧波导板1和内侧波导板2),然后用机械微加工的方法在金属板的相应表面上加工出凹槽11、21,如图2所示。1) First process two metal plates with a certain thickness and 90° bending (
2)将外侧波导板1和内侧波导板2有凹槽的面相对地平行放置,并进一步使凹槽11、21相对应,同时保证两板相对平行。2) Place the grooved surfaces of the
3)打开时域太赫兹波谱系统(TDS系统),将上述制成的如图2所示的太赫兹低损耗弯曲波导接入到TDS系统中合适的位置,使太赫兹信号从太赫兹低损耗弯曲波导一端上的狭缝入射。3) Turn on the time-domain terahertz spectroscopy system (TDS system), and connect the terahertz low-loss curved waveguide made above as shown in Figure 2 to a suitable position in the TDS system, so that the terahertz signal is transmitted from the terahertz low-loss Slit incidence on one end of the curved waveguide.
4)采集数据:使用TDS系统的光电导接收器对太赫兹低损耗弯曲波导的输出信号进行采集。4) Collect data: Use the photoconductive receiver of the TDS system to collect the output signal of the terahertz low-loss curved waveguide.
测试结果表明该太赫兹低损耗弯曲波导输出信号在0.4THz到0.6THz的信号透射率高于95%,这明显优于现有技术中的弯曲波导的损耗。Test results show that the signal transmittance of the output signal of the terahertz low-loss curved waveguide at 0.4 THz to 0.6 THz is higher than 95%, which is obviously better than the loss of the curved waveguide in the prior art.
本发明的太赫兹低损耗弯曲波导结构简单、使用方便、成本低廉。The terahertz low-loss curved waveguide of the invention has the advantages of simple structure, convenient use and low cost.
Claims (10)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310360908.9A CN103457009B (en) | 2013-08-16 | 2013-08-16 | terahertz low-loss curved waveguide |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310360908.9A CN103457009B (en) | 2013-08-16 | 2013-08-16 | terahertz low-loss curved waveguide |
Publications (2)
Publication Number | Publication Date |
---|---|
CN103457009A true CN103457009A (en) | 2013-12-18 |
CN103457009B CN103457009B (en) | 2016-01-20 |
Family
ID=49739141
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201310360908.9A Active CN103457009B (en) | 2013-08-16 | 2013-08-16 | terahertz low-loss curved waveguide |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN103457009B (en) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104183896A (en) * | 2014-08-11 | 2014-12-03 | 电子科技大学 | Four-port device testing structure applicable to terahertz frequency band |
CN104993194A (en) * | 2015-06-24 | 2015-10-21 | 上海理工大学 | Terahertz wave band elimination filtering device |
CN105551920A (en) * | 2016-01-19 | 2016-05-04 | 电子科技大学 | Ultra wide band high-power terahertz radiation source |
CN106154416A (en) * | 2016-08-31 | 2016-11-23 | 欧阳征标 | The controlled unidirectional waveguide of arbitrarily turning round of the No leakage low damage fast mould of magneto-optic thin film magnetic surface |
CN104362419B (en) * | 2014-11-28 | 2017-02-01 | 桂林电子科技大学 | Ultra-wideband (UWB) manual surface plasmonpolariton bend waveguide |
CN107065069A (en) * | 2017-05-12 | 2017-08-18 | 深圳市太赫兹科技创新研究院 | Terahertz beam splitter |
CN107069153A (en) * | 2017-04-12 | 2017-08-18 | 北京大学 | One kind is based on surface plasmons waveguide bend mode converter and its implementation |
WO2018041186A1 (en) * | 2016-08-31 | 2018-03-08 | 深圳大学 | Magnetic surface fast-mode arbitrary-angle unidirectional bent waveguide with low-loss magneto-optical gap |
CN110133855A (en) * | 2019-05-08 | 2019-08-16 | 上海理工大学 | Diffraction-free transmission of terahertz waves based on plasma column arrays |
WO2019179095A1 (en) * | 2018-03-22 | 2019-09-26 | 华为技术有限公司 | Mode conversion device and signal transmission system |
CN113346211A (en) * | 2021-06-04 | 2021-09-03 | 北京邮电大学 | Electromagnetic wave transmission waveguide |
CN116430510A (en) * | 2023-06-14 | 2023-07-14 | 之江实验室 | Optical waveguide and optical waveguide design method |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101038978A (en) * | 2006-12-25 | 2007-09-19 | 北京交通大学 | Non-symmetric structure grid velocity compensation method and velocity compensation-type bending coplane waveguide |
CN101118302A (en) * | 2007-07-30 | 2008-02-06 | 厦门大学 | A long-range surface plasmon waveguide for integrated optical circuit and its manufacturing method |
US20090273532A1 (en) * | 2008-05-02 | 2009-11-05 | William Marsh Rice University | Ultra Low Loss Waveguide for Broadband Terahertz Radiation |
KR101039126B1 (en) * | 2010-01-22 | 2011-06-07 | 한국해양대학교 산학협력단 | Terahertz Wave Parallel Plate Waveguide |
CN103197374A (en) * | 2013-03-12 | 2013-07-10 | 东南大学 | Planar two-waveband surface plasmon waveguide based on composite cycle structure |
-
2013
- 2013-08-16 CN CN201310360908.9A patent/CN103457009B/en active Active
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101038978A (en) * | 2006-12-25 | 2007-09-19 | 北京交通大学 | Non-symmetric structure grid velocity compensation method and velocity compensation-type bending coplane waveguide |
CN101118302A (en) * | 2007-07-30 | 2008-02-06 | 厦门大学 | A long-range surface plasmon waveguide for integrated optical circuit and its manufacturing method |
US20090273532A1 (en) * | 2008-05-02 | 2009-11-05 | William Marsh Rice University | Ultra Low Loss Waveguide for Broadband Terahertz Radiation |
KR101039126B1 (en) * | 2010-01-22 | 2011-06-07 | 한국해양대학교 산학협력단 | Terahertz Wave Parallel Plate Waveguide |
CN103197374A (en) * | 2013-03-12 | 2013-07-10 | 东南大学 | Planar two-waveband surface plasmon waveguide based on composite cycle structure |
Non-Patent Citations (3)
Title |
---|
余春燕: "基于金属周期槽阵列的太赫兹带阻滤波器", 《激光与红外》, vol. 43, no. 7, 31 July 2013 (2013-07-31), pages 803 - 808 * |
袁海军: "等离子体加载的双平板慢波传输线中太赫兹波特性研究", 《电子科技大学硕士学位论文》, 1 April 2012 (2012-04-01), pages 1 - 21 * |
钟任斌: "太赫兹传输线研究", 《电子科技大学博士学位论文》, 31 December 2012 (2012-12-31) * |
Cited By (15)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104183896B (en) * | 2014-08-11 | 2016-11-09 | 电子科技大学 | Four-port device test structure for terahertz frequency band |
CN104183896A (en) * | 2014-08-11 | 2014-12-03 | 电子科技大学 | Four-port device testing structure applicable to terahertz frequency band |
CN104362419B (en) * | 2014-11-28 | 2017-02-01 | 桂林电子科技大学 | Ultra-wideband (UWB) manual surface plasmonpolariton bend waveguide |
CN104993194A (en) * | 2015-06-24 | 2015-10-21 | 上海理工大学 | Terahertz wave band elimination filtering device |
CN105551920A (en) * | 2016-01-19 | 2016-05-04 | 电子科技大学 | Ultra wide band high-power terahertz radiation source |
CN106154416B (en) * | 2016-08-31 | 2021-02-19 | 深圳大学 | Controllable one-way arbitrary turning waveguide of no-leakage low-loss magneto-optical film magnetic surface fast mode |
CN106154416A (en) * | 2016-08-31 | 2016-11-23 | 欧阳征标 | The controlled unidirectional waveguide of arbitrarily turning round of the No leakage low damage fast mould of magneto-optic thin film magnetic surface |
WO2018041186A1 (en) * | 2016-08-31 | 2018-03-08 | 深圳大学 | Magnetic surface fast-mode arbitrary-angle unidirectional bent waveguide with low-loss magneto-optical gap |
CN107069153A (en) * | 2017-04-12 | 2017-08-18 | 北京大学 | One kind is based on surface plasmons waveguide bend mode converter and its implementation |
CN107065069A (en) * | 2017-05-12 | 2017-08-18 | 深圳市太赫兹科技创新研究院 | Terahertz beam splitter |
WO2019179095A1 (en) * | 2018-03-22 | 2019-09-26 | 华为技术有限公司 | Mode conversion device and signal transmission system |
CN110133855A (en) * | 2019-05-08 | 2019-08-16 | 上海理工大学 | Diffraction-free transmission of terahertz waves based on plasma column arrays |
CN113346211A (en) * | 2021-06-04 | 2021-09-03 | 北京邮电大学 | Electromagnetic wave transmission waveguide |
CN116430510A (en) * | 2023-06-14 | 2023-07-14 | 之江实验室 | Optical waveguide and optical waveguide design method |
CN116430510B (en) * | 2023-06-14 | 2023-09-05 | 之江实验室 | Optical waveguide and optical waveguide design method |
Also Published As
Publication number | Publication date |
---|---|
CN103457009B (en) | 2016-01-20 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103457009A (en) | Terahertz low-loss bent waveguide | |
Xie et al. | Wavefront modulation and subwavelength diffractive acoustics with an acoustic metasurface | |
Li et al. | Reflected wavefront manipulation based on ultrathin planar acoustic metasurfaces | |
Tang et al. | Anomalous refraction of airborne sound through ultrathin metasurfaces | |
Liang et al. | Space-coiling metamaterials with double negativity and conical dispersion | |
Mendis et al. | THz interconnect with low-loss and low-group velocity dispersion | |
Chen et al. | Enhanced acoustic sensing through wave compression and pressure amplification in anisotropic metamaterials | |
Zangeneh-Nejad et al. | Performing mathematical operations using high-index acoustic metamaterials | |
Lee et al. | Extreme stiffness hyperbolic elastic metamaterial for total transmission subwavelength imaging | |
Xu et al. | Goos-Hänchen effect in epsilon-near-zero metamaterials | |
Zhao et al. | Beam path and focusing of flexural Lamb waves within phononic crystal-based acoustic lenses | |
Peña et al. | The single-channel regime of transport through random media | |
Patimisco et al. | Low-loss hollow waveguide fibers for mid-infrared quantum cascade laser sensing applications | |
Merklein et al. | On-chip broadband nonreciprocal light storage | |
US8259022B2 (en) | Ultra low loss waveguide for broadband Terahertz radiation | |
WO2015178982A9 (en) | Methods and apparatus for broadband angular selectivity of electromagnetic waves | |
Ai et al. | Multi-beam steering for 6G communications based on graphene metasurfaces | |
Rakich et al. | Quantum theory of continuum optomechanics | |
WO2014139067A1 (en) | Cylindrical electromagnetic wave cloaking device | |
Zhang et al. | Topologically crafted spatiotemporal vortices in acoustics | |
Liu et al. | All-angle negative reflection with an ultrathin acoustic gradient metasurface: Floquet-Bloch modes perspective and experimental verification | |
Henriksson et al. | An approach to ring resonator biosensing assisted by dielectrophoresis: design, simulation and fabrication | |
JP5098895B2 (en) | Terahertz wave generation apparatus and terahertz wave generation method | |
Lin et al. | Subtle application of electrical field-induced lossy mode resonance to enhance performance of optical planar waveguide biosensor | |
Gupta et al. | Asymmetric light reflection at the reflecting layer incorporated in a linear, time-independent and non-magnetic two-dimensional photonic crystal |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant |