CN111400848A - Antenna Design Method for Terahertz Wave Detector Based on Field Effect Transistor - Google Patents
Antenna Design Method for Terahertz Wave Detector Based on Field Effect Transistor Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及平面集成天线的设计领域,具体涉及一种基于场效应晶体管的太赫兹波探测器的天线设计方法。The invention relates to the design field of a plane integrated antenna, in particular to an antenna design method of a terahertz wave detector based on a field effect transistor.
背景技术Background technique
太赫兹波是频率在0.1THz-10THz的电磁波,介于红外和毫米波之间,在电磁波谱中处于重要的位置。太赫兹波由于具有透射性强、电离能量小、频带宽、分辨率高、相干性强等特点,在材料特性表征、高分辨率成像、医学诊断、安全检查、信息通讯、雷达探测、大气与环境检测等众多领域有着极其重要的应用。因而,近些年来,太赫兹波段吸引着越来越多的关注与研究。基于场效应晶体管的太赫兹波探测器始于1993年Dyakonov和Shur提出等离子体波理论,随后实际的器件在不同的材料上被研制出来。由于具有体积小、易于与芯片集成、响应速度快、室温工作等特点,这种太赫兹波探测器已经成为一种主流的太赫兹波探测手段。Terahertz waves are electromagnetic waves with a frequency of 0.1THz-10THz, between infrared and millimeter waves, and occupy an important position in the electromagnetic spectrum. Terahertz waves are widely used in material characterization, high-resolution imaging, medical diagnosis, security inspection, information communication, radar detection, atmospheric and Environmental detection and many other fields have extremely important applications. Therefore, in recent years, the terahertz band has attracted more and more attention and research. Terahertz wave detectors based on field effect transistors began with the plasma wave theory proposed by Dyakonov and Shur in 1993, and then actual devices were developed on different materials. Due to its small size, easy integration with chips, fast response speed, and room temperature operation, this terahertz wave detector has become a mainstream terahertz wave detection method.
通常为了进一步提高探测器的响应度,基于场效应晶体管的太赫兹波探测器通过在源极和栅极外接平面天线的方式来耦合空间中的太赫兹波,从而在栅源电极之间产生一交流信号,这一交流信号可以调制晶体管沟道中的等离子体波,最终在晶体管漏极与源极之间产生直流的太赫兹响应信号。显然,合理的天线设计可以增强太赫兹波与晶体管之间的耦合效率,从而进一步提高探测的响应度。基于天线的互易性,接收模式下天线的特性参数与发射模式下的天线相同。因而,传统的天线设计大多也是基于天线在发射模式下的电磁仿真,通过S参数、辐射效率、增益等来衡量天线的性能。这种仿真,必然涉及到天线源阻抗与天线阻抗的匹配。对于场效应晶体管太赫兹波探测器,晶体管的栅源电极之间的输入阻抗可以视为天线仿真中的源阻抗。然而,由于目前场效应晶体管在太赫兹波段缺乏简易准确的输入阻抗提取方式,传统的天线设计方法必然缺乏足够的有效性。Usually, in order to further improve the responsivity of the detector, the terahertz wave detector based on the field effect transistor couples the terahertz wave in space by connecting the source and the gate with a planar antenna, thereby generating a terahertz wave between the gate and source electrodes. The AC signal, which modulates the plasma wave in the transistor channel, ultimately produces a DC terahertz response signal between the transistor drain and source. Obviously, a reasonable antenna design can enhance the coupling efficiency between terahertz waves and transistors, thereby further improving the responsivity of detection. Based on the reciprocity of the antenna, the characteristic parameters of the antenna in the receive mode are the same as those in the transmit mode. Therefore, most of the traditional antenna designs are also based on the electromagnetic simulation of the antenna in the transmitting mode, and the performance of the antenna is measured by S-parameters, radiation efficiency, gain, etc. This kind of simulation must involve the matching of the antenna source impedance and the antenna impedance. For field effect transistor terahertz wave detectors, the input impedance between the gate-source electrodes of the transistor can be regarded as the source impedance in the antenna simulation. However, due to the lack of simple and accurate input impedance extraction methods for field effect transistors in the terahertz band, the traditional antenna design methods must lack sufficient effectiveness.
发明内容SUMMARY OF THE INVENTION
(一)要解决的技术问题(1) Technical problems to be solved
鉴于上述技术问题,本发明提出了一种基于场效应晶体管的太赫兹波探测器的天线设计方法,以至少部分解决上述技术问题。In view of the above technical problems, the present invention proposes an antenna design method for a terahertz wave detector based on field effect transistors to at least partially solve the above technical problems.
(二)技术方案(2) Technical solutions
根据本发明的一方面,提供一种基于场效应晶体管的太赫兹波探测器的天线设计方法,包括:According to an aspect of the present invention, an antenna design method for a terahertz wave detector based on a field effect transistor is provided, including:
构建一太赫兹波探测器模型;Build a terahertz wave detector model;
设置一束频率变化的平面太赫兹波,垂直入射到集成天线的太赫兹波探测器模型上;A beam of planar terahertz waves with varying frequencies is set to be vertically incident on the terahertz wave detector model of the integrated antenna;
提取所述太赫兹波探测器模型的场效应晶体管的沟道中一位置的电场强度;extracting the electric field intensity at a position in the channel of the field effect transistor of the terahertz wave detector model;
计算所述天线在不同频率处产生的电场增强,得到电场增强随频率的变化关系;Calculate the electric field enhancement generated by the antenna at different frequencies, and obtain the variation relationship of the electric field enhancement with frequency;
根据计算得出的所述变化关系获取所述天线的中心频率;Obtain the center frequency of the antenna according to the calculated variation relationship;
根据所述天线的中心频率确定所述天线的结构以及尺寸。The structure and size of the antenna are determined according to the center frequency of the antenna.
在进一步的实施方案中,所述提取电场强度的位置位于所述场效应晶体管的栅极靠近源极一侧边缘的沟道中。In a further embodiment, the location where the electric field strength is extracted is located in the channel on the side edge of the gate of the field effect transistor close to the source.
在进一步的实施方案中,所述构建的太赫兹波探测器模型包括:场效应晶体管和平面天线;其中,所述平面天线分别与所述场效应晶体管的栅极和源极相连。In a further embodiment, the constructed terahertz wave detector model includes: a field effect transistor and a planar antenna; wherein the planar antenna is connected to the gate and source of the field effect transistor, respectively.
在进一步的实施方案中,所述场效应晶体管包括:In further embodiments, the field effect transistor comprises:
衬底;substrate;
缓冲层,置于所述衬底上;a buffer layer, placed on the substrate;
沟道层,置于所述缓冲层上;a channel layer, placed on the buffer layer;
栅介质层,置于所述沟道层上;a gate dielectric layer, placed on the channel layer;
栅极、漏极和源极置于所述栅介质层上,其中所述栅极置于所述漏极和所述源极之间。A gate electrode, a drain electrode and a source electrode are placed on the gate dielectric layer, wherein the gate electrode is placed between the drain electrode and the source electrode.
在进一步的实施方案中,所述提取场效应晶体管一位置的电场强度为:通过在HFSS中的Fields Calculator里面选取ComplexMag_E函数,计算所述位置的电场强度。In a further embodiment, the extraction of the electric field strength at a position of the field effect transistor is: by selecting the ComplexMag_E function in the Fields Calculator in HFSS, the electric field strength at the position is calculated.
在进一步的实施方案中,所述计算不同频率处的电场增强为:将提取的电场强度除以入射太赫兹波的电场强度大小,得到天线在该位置的电场增强。In a further embodiment, the calculation of the electric field enhancement at different frequencies is: dividing the extracted electric field strength by the electric field strength of the incident terahertz wave to obtain the electric field enhancement of the antenna at this position.
在进一步的实施方案中,所述天线的中心频率为所述电场增强随频率的变化关系中的峰值对应的频率。In a further embodiment, the center frequency of the antenna is a frequency corresponding to a peak in the electric field enhancement as a function of frequency.
在进一步的实施方案中,所述场效应晶体管为MOSFET、FINFET、MESFET或HEMT。In further embodiments, the field effect transistor is a MOSFET, FINFET, MESFET or HEMT.
在进一步的实施方案中,所述天线为蝶形天线、偶极子天线或贴片天线。In further embodiments, the antenna is a butterfly antenna, a dipole antenna or a patch antenna.
在进一步的实施方案中,所述根据所述天线的中心频率确定所述天线的结构以及尺寸包括:In a further embodiment, the determining the structure and size of the antenna according to the center frequency of the antenna includes:
根据所述天线的中心频率是否与目标频率一致,调整天线尺寸以使其中心频率与目标频率一致;According to whether the center frequency of the antenna is consistent with the target frequency, adjust the size of the antenna so that the center frequency is consistent with the target frequency;
根据不同结构的天线在中心频率处的电场增强选择电场增强相对较大的天线结构。The antenna structure with relatively large electric field enhancement is selected according to the electric field enhancement at the center frequency of the antennas of different structures.
(三)有益效果(3) Beneficial effects
本发明提供一种基于场效应晶体管的太赫兹波探测器的天线设计方法,利用天线在场效应晶体管栅极边缘下方沟道中的电场增强来表征天线的性能,从而进行有效的场效应晶体管太赫兹波探测器的设计;该方法不用提取场效应晶体管的栅源电极之间的输入阻抗,同时可以直观地与太赫兹波探测器响应度相关联,是一种直观有效的太赫兹天线设计方法。The invention provides an antenna design method for a terahertz wave detector based on a field effect transistor, which utilizes the electric field enhancement of the antenna in the channel below the gate edge of the field effect transistor to characterize the performance of the antenna, so as to carry out effective field effect transistor terahertz wave detection. The design of the detector; the method does not need to extract the input impedance between the gate-source electrodes of the field effect transistor, and can be directly related to the responsivity of the terahertz wave detector. It is an intuitive and effective method for designing a terahertz antenna.
附图说明Description of drawings
图1为本发明实施例构建的集成天线的太赫兹波探测器结构的俯视图。FIG. 1 is a top view of the structure of a terahertz wave detector with an integrated antenna constructed in an embodiment of the present invention.
图2为本发明实施例集成天线的太赫兹波探测器场效应晶体管部分的截面图。FIG. 2 is a cross-sectional view of the field effect transistor part of the terahertz wave detector of the integrated antenna according to the embodiment of the present invention.
图3为本发明实施例基于场效应晶体管的太赫兹波探测器的天线设计方法的流程图。FIG. 3 is a flowchart of an antenna design method for a field effect transistor-based terahertz wave detector according to an embodiment of the present invention.
具体实施方式Detailed ways
为使本发明的目的、技术方案和优点更加清楚明白,以下结合具体实施例,并参照附图,对本发明作进一步的详细说明。In order to make the objectives, technical solutions and advantages of the present invention more clearly understood, the present invention will be further described in detail below in conjunction with specific embodiments and with reference to the accompanying drawings.
根据本发明的一个实施例,提供一种基于场效应晶体管的太赫兹波探测器的天线设计方法,如图3所示包括:According to an embodiment of the present invention, an antenna design method for a field effect transistor-based terahertz wave detector is provided, as shown in FIG. 3 , including:
构建一太赫兹波探测器模型;Build a terahertz wave detector model;
设置一束频率变化的平面太赫兹波,垂直入射到集成天线的太赫兹波探测器模型上;A beam of planar terahertz waves with varying frequencies is set to be vertically incident on the terahertz wave detector model of the integrated antenna;
提取所述太赫兹波探测器模型的场效应晶体管的沟道中一位置的电场强度;extracting the electric field intensity at a position in the channel of the field effect transistor of the terahertz wave detector model;
计算所述天线在不同频率处产生的电场增强,得到电场增强随频率的变化关系;Calculate the electric field enhancement generated by the antenna at different frequencies, and obtain the variation relationship of the electric field enhancement with frequency;
根据计算得出的所述变化关系获取所述天线的中心频率;Obtain the center frequency of the antenna according to the calculated variation relationship;
根据所述天线的中心频率确定所述天线的结构以及尺寸。The structure and size of the antenna are determined according to the center frequency of the antenna.
其中,在选择合适的结构以及尺寸的步骤中,根据计算得出的所述变化关系可以获取天线的中心频率,进而根据目标频率调整天线的尺寸,并比较不同结构类型的天线在沟道中电场增强的相对大小,从而在太赫兹波探测器天线设计中选择合适的结构以及尺寸。Wherein, in the step of selecting a suitable structure and size, the center frequency of the antenna can be obtained according to the calculated variation relationship, and then the size of the antenna can be adjusted according to the target frequency, and the electric field enhancement in the channel of the antenna with different structure types can be compared. The relative size of the terahertz wave detector can be used to select the appropriate structure and size in the design of the terahertz wave detector antenna.
其中,所述根据所述天线的中心频率确定所述天线的结构以及尺寸包括:根据所述天线的中心频率是否与目标频率一致,调整天线尺寸以使其中心频率与目标频率一致;根据不同结构的天线在中心频率处的电场增强选择电场增强相对较大的天线结构。The determining the structure and size of the antenna according to the center frequency of the antenna includes: adjusting the size of the antenna to make the center frequency consistent with the target frequency according to whether the center frequency of the antenna is consistent with the target frequency; The electric field enhancement of the antenna at the center frequency selects an antenna structure with a relatively large electric field enhancement.
在本实施例中,电场增强随频率的变化关系中的峰值对应的频率位置表征天线的中心频率;电场增强峰值的相对大小表征不同天线的接收性能,即耦合太赫兹波,并转化为太赫兹响应的能力,其直接与太赫兹响应度的大小相关联。In this embodiment, the frequency position corresponding to the peak in the relationship between the electric field enhancement and frequency represents the center frequency of the antenna; the relative magnitude of the electric field enhancement peak represents the receiving performance of different antennas, that is, the coupled terahertz waves are converted into terahertz waves The ability to respond, which is directly related to the magnitude of the terahertz responsivity.
本发明利用天线在场效应晶体管栅极边缘下方沟道中的电场增强来表征太赫兹天线的性能,并且可以和太赫兹波探测器的响应度相关联。具体来说,基于场效应晶体管的太赫兹波探测器一般通过在源极和栅极外接平面天线的方式来耦合空间中的太赫兹波,进而可以调制场效应晶体管沟道中的等离子体波,最终在场效应晶体管漏极与源极之间产生直流的太赫兹响应信号。本发明利用天线在场效应晶体管栅极边缘下方沟道中的电场增强来表征天线的这种调制作用,从而进行有效的太赫兹天线设计。The invention utilizes the electric field enhancement of the antenna in the channel below the gate edge of the field effect transistor to characterize the performance of the terahertz antenna, and can be correlated with the responsivity of the terahertz wave detector. Specifically, terahertz wave detectors based on field effect transistors generally couple the terahertz waves in space by externally connecting planar antennas to the source and gate, so as to modulate the plasma wave in the channel of the field effect transistor, and finally A DC terahertz response signal is generated between the drain and source of the field effect transistor. The present invention utilizes the electric field enhancement of the antenna in the channel below the gate edge of the field effect transistor to characterize this modulation effect of the antenna, so as to carry out effective terahertz antenna design.
本发明的所述天线设计方法,和具体采用的天线结构和尺寸无关;和天线的具体工作频率无关(覆盖一切电磁波的波段);和具体采用的场效应晶体管探测器的结构无关;和具体采用的天线与场效应晶体管的连接方式无关。The antenna design method of the present invention has nothing to do with the specific antenna structure and size; has nothing to do with the specific operating frequency of the antenna (covering all electromagnetic wave bands); has nothing to do with the structure of the field effect transistor detector specifically used; The antenna has nothing to do with how the FET is connected.
在本实施例中,所述构建的太赫兹波探测器指的是一切形式的场效应晶体管探测器,包括但是不限于MOSFET、FINFET、MESFET、HEMT等等。In this embodiment, the constructed terahertz wave detector refers to all forms of field effect transistor detectors, including but not limited to MOSFET, FINFET, MESFET, HEMT and so on.
在本实施例中,所述天线种类指的是一切形式的平面天线种类,包括但是不限于:蝶形天线,偶极子天线,贴片天线等等。In this embodiment, the antenna types refer to all types of planar antennas, including but not limited to: butterfly antennas, dipole antennas, patch antennas, and the like.
在本实施例中,所述构建的太赫兹波探测器模型包括:场效应晶体管和平面天线;其中,所述平面天线分别与所述场效应晶体管的栅极和源极相连。In this embodiment, the constructed terahertz wave detector model includes: a field effect transistor and a planar antenna; wherein the planar antenna is connected to the gate and source of the field effect transistor, respectively.
在本实施例中,所述场效应晶体管如图2所示包括:In this embodiment, the field effect transistor as shown in FIG. 2 includes:
衬底10;
缓冲层9,置于所述衬底10上;The buffer layer 9 is placed on the
沟道层8,置于所述缓冲层9上;The
栅介质层7,置于所述沟道层8上;The
其中,如图1所示所述栅极1、漏极2和源极5置于所述栅介质层7上,其中所述栅极1置于所述漏极2和所述源极5之间。Wherein, as shown in FIG. 1 , the
在本实施例中,所述构建的太赫兹波探测器模型使用的仿真和计算方法可以是一切形式的仿真和计算方法,包括但是不限于:MATLAB、HFSS、COMSEL等仿真软件(或者FEM、FDTD和MOM等仿真算法)。In this embodiment, the simulation and calculation method used in the constructed terahertz wave detector model may be any form of simulation and calculation method, including but not limited to: MATLAB, HFSS, COMSEL and other simulation software (or FEM, FDTD, etc. and simulation algorithms such as MOM).
在本实施例中,所述提取场效应晶体管栅极靠近源极一侧边缘下方沟道中的电场强度为:通过在HFSS中的Fields Calculator里面选取ComplexMag_E函数,选取场效应晶体管栅极靠近源极一侧边缘下方沟道的特定位置提取该处的电场强度。In this embodiment, the extraction of the electric field strength in the channel below the edge of the FET gate close to the source is: by selecting the ComplexMag_E function in the Fields Calculator in HFSS, selecting the FET gate close to the source a A specific location of the channel below the side edge extracts the electric field strength there.
在本实施例中,所述计算不同频点处的电场增强为:将提取的电场强度除以入射太赫兹波的电场强度大小,得到天线在该处的电场增强。In this embodiment, the calculation of the electric field enhancement at different frequency points is as follows: dividing the extracted electric field strength by the electric field strength of the incident terahertz wave to obtain the electric field enhancement of the antenna at that position.
针对基于场效应晶体管的太赫兹波探测器的特殊原理,其耦合在栅源电极之间的交流信号的主要作用是调制场效应晶体管沟道中的等离子体波,天线在沟道中产生的电场必然发挥着十分重要的作用。因此,本发明提出一种利用天线在场效应晶体管栅极边缘下方沟道中的电场增强来表征天线的性能,从而进行有效的场效应晶体管太赫兹波探测器的设计。Aiming at the special principle of terahertz wave detectors based on field effect transistors, the main function of the AC signal coupled between the gate-source electrodes is to modulate the plasma wave in the channel of the field effect transistor, and the electric field generated by the antenna in the channel must play a role. plays a very important role. Therefore, the present invention proposes a method to characterize the performance of the antenna by using the electric field enhancement of the antenna in the channel below the gate edge of the field effect transistor, so as to carry out the design of an effective field effect transistor terahertz wave detector.
需要说明的是,本文可提供包含特定值的参数的示范,但这些参数无需确切等于相应的值,而是可在可接受的误差容限或设计约束内近似于相应值。实施例中提到的方向用语,例如“上”、“下”、“前”、“后”、“左”、“右”等,仅是参考附图的方向,并非用来限制本发明的保护范围。此外,除非特别描述或必须依序发生的步骤,上述步骤的顺序并无限制于以上所列,且可根据所需设计而变化或重新安排。并且上述实施例可基于设计及可靠度的考虑,彼此混合搭配使用或与其他实施例混合搭配使用,即不同实施例中的技术特征可以自由组合形成更多的实施例。It should be noted that demonstrations of parameters including specific values may be provided herein, but these parameters need not be exactly equal to the corresponding values, but may be approximated within acceptable error tolerances or design constraints. The directional terms mentioned in the embodiments, such as "up", "down", "front", "rear", "left", "right", etc., are only for referring to the directions of the drawings, and are not intended to limit the present invention. protected range. Furthermore, unless the steps are specifically described or must occur sequentially, the order of the above steps is not limited to those listed above, and may be varied or rearranged according to the desired design. And the above embodiments can be mixed and matched with each other or with other embodiments based on the consideration of design and reliability, that is, the technical features in different embodiments can be freely combined to form more embodiments.
以上所述的具体实施例,对本发明的目的、技术方案和有益效果进行了进一步详细说明,应理解的是,以上所述仅为本发明的具体实施例而已,并不用于限制本发明,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The specific embodiments described above further describe the purpose, technical solutions and beneficial effects of the present invention in detail. It should be understood that the above-mentioned specific embodiments are only specific embodiments of the present invention, and are not intended to limit the present invention. Within the spirit and principle of the present invention, any modifications, equivalent replacements, improvements, etc. made should be included within the protection scope of the present invention.
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN112531071A (en) * | 2020-12-18 | 2021-03-19 | 中国科学院苏州纳米技术与纳米仿生研究所 | Terahertz field effect detector based on thin barrier material and design method thereof |
| CN113639866A (en) * | 2021-08-25 | 2021-11-12 | 中国科学院苏州纳米技术与纳米仿生研究所 | Field Effect Broad Spectrum Detector |
| CN113656929A (en) * | 2021-06-11 | 2021-11-16 | 中国船舶重工集团公司第七二三研究所 | Simulation method of terahertz reflective phase shifter based on tunable liquid crystal material |
| CN113764858A (en) * | 2021-08-27 | 2021-12-07 | 西安交通大学 | Graphene-based antenna-enhanced terahertz detector and preparation method thereof |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102299174A (en) * | 2010-06-23 | 2011-12-28 | 电力集成公司 | Layout design for a high power, GaN-based FET |
| CN103035706A (en) * | 2013-01-04 | 2013-04-10 | 电子科技大学 | Vertical gallium nitride based nitride heterojunction field effect transistor with polarized doped current barrier layer |
| CN104538742A (en) * | 2015-01-09 | 2015-04-22 | 中国电子科技集团公司第三十八研究所 | Circular polarization waveguide slot antenna and design method thereof |
| CN104916732A (en) * | 2014-03-12 | 2015-09-16 | 中国科学院苏州纳米技术与纳米仿生研究所 | Graphene terahertz wave detector and manufacturing method thereof |
| CN105549227A (en) * | 2015-12-18 | 2016-05-04 | 成都浩博依科技有限公司 | Terahertz wave space external modulator based on GaN semiconductor material heterojunction field-effect transistor structure |
-
2018
- 2018-12-27 CN CN201811616335.0A patent/CN111400848A/en active Pending
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102299174A (en) * | 2010-06-23 | 2011-12-28 | 电力集成公司 | Layout design for a high power, GaN-based FET |
| CN103035706A (en) * | 2013-01-04 | 2013-04-10 | 电子科技大学 | Vertical gallium nitride based nitride heterojunction field effect transistor with polarized doped current barrier layer |
| CN104916732A (en) * | 2014-03-12 | 2015-09-16 | 中国科学院苏州纳米技术与纳米仿生研究所 | Graphene terahertz wave detector and manufacturing method thereof |
| CN104538742A (en) * | 2015-01-09 | 2015-04-22 | 中国电子科技集团公司第三十八研究所 | Circular polarization waveguide slot antenna and design method thereof |
| CN105549227A (en) * | 2015-12-18 | 2016-05-04 | 成都浩博依科技有限公司 | Terahertz wave space external modulator based on GaN semiconductor material heterojunction field-effect transistor structure |
Non-Patent Citations (6)
| Title |
|---|
| [加拿大]DARYOOSH SAEEDKIA: "《太赫兹成像传感及通信技术手册》", 31 May 2016 * |
| WOJCIECH KNAP等: "Terahertz imaging with GaAs and GaN plasma field effect transistors detectors", 《2016 MIXDES - 23RD INTERNATIONAL CONFERENCE MIXED DESIGN OF INTEGRATED CIRCUITS AND SYSTEMS》 * |
| 岳峥: "RFID读写器及标签的天线研究与设计", 《中国优秀硕士学位论文全文数据库 信息科技辑》 * |
| 张博文等: "基于场效应晶体管的太赫兹探测器中天线设计的一种有效方法", 《红外与毫米波学报》 * |
| 杨永侠等: "基于Zigbee的一种矩形微带天线的设计", 《西安工业大学学报》 * |
| 柳培忠等: "《微波电路和无线系统的仿真与设计》", 30 June 2015 * |
Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN112531071A (en) * | 2020-12-18 | 2021-03-19 | 中国科学院苏州纳米技术与纳米仿生研究所 | Terahertz field effect detector based on thin barrier material and design method thereof |
| CN113656929A (en) * | 2021-06-11 | 2021-11-16 | 中国船舶重工集团公司第七二三研究所 | Simulation method of terahertz reflective phase shifter based on tunable liquid crystal material |
| CN113656929B (en) * | 2021-06-11 | 2024-05-03 | 中国船舶重工集团公司第七二三研究所 | Simulation method of terahertz reflection phase shifter based on tunable liquid crystal material |
| CN113639866A (en) * | 2021-08-25 | 2021-11-12 | 中国科学院苏州纳米技术与纳米仿生研究所 | Field Effect Broad Spectrum Detector |
| CN113639866B (en) * | 2021-08-25 | 2024-05-28 | 中国科学院苏州纳米技术与纳米仿生研究所 | Field Effect Broadband Detector |
| CN113764858A (en) * | 2021-08-27 | 2021-12-07 | 西安交通大学 | Graphene-based antenna-enhanced terahertz detector and preparation method thereof |
| CN113764858B (en) * | 2021-08-27 | 2023-05-02 | 西安交通大学 | Antenna-enhanced terahertz detector based on graphene and preparation method thereof |
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