[go: up one dir, main page]

CN216488081U - Near-infrared response thermal electron photoelectric detector - Google Patents

Near-infrared response thermal electron photoelectric detector Download PDF

Info

Publication number
CN216488081U
CN216488081U CN202123202776.6U CN202123202776U CN216488081U CN 216488081 U CN216488081 U CN 216488081U CN 202123202776 U CN202123202776 U CN 202123202776U CN 216488081 U CN216488081 U CN 216488081U
Authority
CN
China
Prior art keywords
film
layer
thin film
thickness
infrared
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
CN202123202776.6U
Other languages
Chinese (zh)
Inventor
龙拥兵
梁文跃
徐海涛
邓海东
兰玉彬
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.)
South China Agricultural University
Original Assignee
South China Agricultural University
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 South China Agricultural University filed Critical South China Agricultural University
Priority to CN202123202776.6U priority Critical patent/CN216488081U/en
Application granted granted Critical
Publication of CN216488081U publication Critical patent/CN216488081U/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Light Receiving Elements (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

本实用新型公开一种近红外响应的热电子光电探测器,该热电子光电探测器包括自下而上排列的第一电极层薄膜、第一电极连接层薄膜、基底、金属连接层、金属层薄膜和一维光子晶体;所述金属层薄膜上设置有第二电极;所述一维光子晶体由均匀薄膜介质周期性交替排列而成。该热电子光电探测器能够有效拓展硅基光电探测器件的近红外吸收能力,实现近红外波长区域的有效响应。

Figure 202123202776

The utility model discloses a thermal electron photodetector with near-infrared response. The thermal electron photodetector comprises a first electrode layer thin film, a first electrode connecting layer thin film, a substrate, a metal connecting layer and a metal layer arranged from bottom to top. A thin film and a one-dimensional photonic crystal; the metal layer thin film is provided with a second electrode; the one-dimensional photonic crystal is formed by a uniform thin film medium periodically alternately arranged. The thermionic photodetector can effectively expand the near-infrared absorption capability of the silicon-based photodetector device, and realize an effective response in the near-infrared wavelength region.

Figure 202123202776

Description

一种近红外响应的热电子光电探测器A near-infrared responsive thermionic photodetector

技术领域technical field

本实用新型涉及光电探测,具体涉及一种近红外响应的热电子光电探测器。The utility model relates to photoelectric detection, in particular to a thermal electron photoelectric detector with near-infrared response.

背景技术Background technique

光电探测器作为光学传感器的一种,可以将光信号转换成电信号,被广泛应用于在军事和国民经济中,如航空航天、光通信、工业控制、近红外成像等领域,如光纤通信、生物模式识别、无人驾驶和无人机、光电耦合器等技术中。As a kind of optical sensor, photodetectors can convert optical signals into electrical signals, and are widely used in military and national economy, such as aerospace, optical communication, industrial control, near-infrared imaging and other fields, such as optical fiber communication, Biometric pattern recognition, unmanned and unmanned aerial vehicles, optocouplers and other technologies.

其中,硅(Si)材料因成本低、纯度高、微纳加工工艺成熟、集成度高、器件特性好等优点,被广泛地应用于在可见光波段的光器件。然而,由于Si的禁带宽度为1.12eV,吸收谱在1100nm处截止,因此,Si的吸收波长范围在400nm到1100nm之间,无法直接应用于近红外光电探测。Among them, silicon (Si) materials are widely used in optical devices in the visible light band due to their advantages of low cost, high purity, mature micro-nano processing technology, high integration, and good device characteristics. However, since the forbidden band width of Si is 1.12 eV and the absorption spectrum is cut off at 1100 nm, the absorption wavelength range of Si is between 400 nm and 1100 nm, which cannot be directly applied to near-infrared photodetection.

实用新型内容Utility model content

本实用新型的目的在于克服上述存在的问题,提供一种近红外响应的热电子光电探测器,该热电子光电探测器能够有效拓展硅基光电探测器件的近红外吸收能力,实现近红外波长区域的有效响应。The purpose of this utility model is to overcome the above-mentioned problems, and to provide a near-infrared-responsive thermionic photodetector, which can effectively expand the near-infrared absorption capability of the silicon-based photoelectric detection device and realize the near-infrared wavelength region. a valid response.

本实用新型的目的通过以下技术方案实现:The purpose of the present utility model is achieved through the following technical solutions:

一种近红外响应的热电子光电探测器,包括自下而上排列的第一电极层薄膜、第一电极连接层薄膜、基底、金属连接层、金属层薄膜和一维光子晶体;所述金属层薄膜上设置有第二电极。A near-infrared response thermionic photodetector, comprising a first electrode layer film, a first electrode connection layer film, a substrate, a metal connection layer, a metal layer film and a one-dimensional photonic crystal arranged from bottom to top; the metal A second electrode is arranged on the layer film.

上述近红外响应的热电子光电探测器的工作原理为:The working principle of the above NIR-responsive thermionic photodetector is as follows:

通过在传统的金属/Si结构肖特基光电探测器的基础上,使用一维光子晶体优化光电探测器的性能。由于一维光子晶体与金属层薄膜之间存在TPP模式,入射光照射在探测器表面时,形成热电子,热电子注入Si基底形成光电流,从而显著提升热电子光电探测器在近红外波段的吸收响应能力。The performance of the photodetector is optimized by using a one-dimensional photonic crystal based on the traditional metal/Si structure Schottky photodetector. Due to the existence of the TPP mode between the one-dimensional photonic crystal and the metal layer film, when the incident light irradiates the surface of the detector, hot electrons are formed, and the hot electrons are injected into the Si substrate to form a photocurrent, thereby significantly improving the thermal electron photodetector in the near-infrared band. Absorb responsiveness.

本实用新型的一个优选方案,其中,所述一维光子晶体由均匀薄膜介质周期性交替排列而成。In a preferred solution of the present invention, the one-dimensional photonic crystals are formed by periodically alternately arranging uniform thin film media.

进一步,所述一维光子晶体的薄膜介质为TiO2和SiO2Further, the thin film medium of the one-dimensional photonic crystal is TiO 2 and SiO 2 .

本实用新型的一个优选方案,其中,所述一维光子晶体的排列周期为5至10个周期,每一周期包括一层TiO2薄膜和一层SiO2薄膜;所述一维光子晶体的周期的厚度为364nm至424nm。In a preferred solution of the present invention, the one-dimensional photonic crystal has an arrangement period of 5 to 10 periods, and each period includes a layer of TiO 2 thin film and a layer of SiO 2 thin film; the period of the one-dimensional photonic crystal is The thickness is 364nm to 424nm.

进一步,一层TiO2薄膜的厚度为146nm至171nm;一层SiO2薄膜的厚度为218nm至253nm。Further, the thickness of one layer of TiO 2 thin film is 146 nm to 171 nm; the thickness of one layer of SiO 2 thin film is 218 nm to 253 nm.

通过调控一维光子晶体的周期数、周期中TiO2薄膜厚度和SiO2薄膜厚度,实现对光电探测器吸收波长的选择;此外,还可以通过调控金属层薄膜的厚度,实现对光电探测器最优吸收率的有效调控。The selection of the absorption wavelength of the photodetector can be achieved by adjusting the number of periods of the one-dimensional photonic crystal, the thickness of the TiO 2 film and the thickness of the SiO 2 film in the period. Effective control of optimal absorption rate.

本实用新型的一个优选方案,其中,所述基底为单晶Si晶片;所述金属连接层为Ti薄膜,厚度为0.5nm;所述金属层为Au薄膜,厚度为10nm至35nm。In a preferred solution of the present invention, the substrate is a single crystal Si wafer; the metal connection layer is a Ti film with a thickness of 0.5 nm; the metal layer is an Au film with a thickness of 10 nm to 35 nm.

本实用新型的一个优选方案,其中,所述第一电极连接层为Ti薄膜,厚度为30nm至50nm;所述第一电极层为Au薄膜,厚度为20nm至100nm。In a preferred solution of the present invention, the first electrode connecting layer is a Ti film with a thickness of 30 nm to 50 nm; the first electrode layer is an Au film with a thickness of 20 nm to 100 nm.

本实用新型与现有技术相比具有以下有益效果:Compared with the prior art, the utility model has the following beneficial effects:

在传统的金属/Si结构肖特基光电探测器的基础上,使用一维光子晶体优化光电探测器的性能,由于一维光子晶体与金属层薄膜之间存在TPP模式,入射光照射在探测器表面时,形成热电子,热电子注入Si基底形成光电流,从而显著提升热电子光电探测器在近红外波段的吸收响应能力,可用于探测能量低于半导体禁带的可见光和近红外光。On the basis of the traditional metal/Si structure Schottky photodetector, a one-dimensional photonic crystal is used to optimize the performance of the photodetector. Since there is a TPP mode between the one-dimensional photonic crystal and the metal layer film, the incident light irradiates the detector. On the surface, thermionic electrons are formed, and thermionic electrons are injected into the Si substrate to form a photocurrent, thereby significantly improving the absorption response capability of thermionic photodetectors in the near-infrared band, and can be used to detect visible light and near-infrared light with energy lower than the semiconductor band gap.

附图说明Description of drawings

图1为本实用新型的近红外响应的热电子光电探测器的结构示意图。1 is a schematic structural diagram of a near-infrared response thermionic photodetector of the present invention.

图2为本实用新型的热电子光电探测器的第一种具体实施方式给定Tamm耦合中心波长为1300nm、1400nm、1500nm、1600nm和1700nm的光电探测器器件的净吸收率光谱图。FIG. 2 is the net absorptivity spectrogram of the photodetector devices with Tamm coupling center wavelengths of 1300 nm, 1400 nm, 1500 nm, 1600 nm and 1700 nm in the first embodiment of the thermionic photodetector of the present invention.

图3为本实用新型的热电子光电探测器的第一种具体实施方式的中心波长为1500nm的不同Au层厚度的光电探测器器件的吸收率对比图。FIG. 3 is a comparison diagram of absorptivity of photodetector devices with different Au layer thicknesses having a center wavelength of 1500 nm according to the first specific embodiment of the thermionic photodetector of the present invention.

图4为本实用新型的热电子光电探测器的第二种具体实施方式在0V偏压和-1V偏压下的响应度谱。FIG. 4 is the responsivity spectrum of the second embodiment of the thermionic photodetector of the present invention under 0V bias and -1V bias.

图5为本实用新型的热电子光电探测器的第三种具体实施方式在0V偏压和-1V偏压下的响应度谱。FIG. 5 is the responsivity spectrum of the third embodiment of the thermionic photodetector of the present invention under 0V bias and -1V bias.

具体实施方式Detailed ways

为了使本领域的技术人员很好地理解本实用新型的技术方案,下面结合实施例和附图对本实用新型作进一步描述,但本实用新型的实施方式不仅限于此。In order for those skilled in the art to better understand the technical solutions of the present invention, the present invention will be further described below with reference to the embodiments and accompanying drawings, but the embodiments of the present invention are not limited thereto.

实施例1Example 1

参见图1,本实施例的近红外响应的热电子光电探测器,包括自下而上依次排列的第一电极层薄膜1、第一电极连接层薄膜2、基底3、金属连接层4、金属层薄膜5和一维光子晶体6;所述金属层薄膜5上设置有第二电极51。Referring to FIG. 1 , the near-infrared response thermionic photodetector of this embodiment includes a first electrode layer film 1 , a first electrode connection layer film 2 , a substrate 3 , a metal connection layer 4 , and a metal connection layer 4 , which are sequentially arranged from bottom to top layer film 5 and one-dimensional photonic crystal 6; the metal layer film 5 is provided with a second electrode 51.

在本实施例中,所述一维光子晶体6由均匀介质薄膜周期性交替排列而成,薄膜介质分别为TiO2(二氧化钛)和SiO2(二氧化硅)。一维光子晶体的排列周期为5至10个周期,每一周期包括一层TiO2薄膜和一层SiO2薄膜;一层TiO2薄膜的厚度为146nm至171nm,所述一层SiO2薄膜的厚度为218nm至253nm;所述一维光子晶体周期的厚度为364nm至424nm。其中,所述一维光子晶体周期中的一维光子晶体的禁带中心波长,可以通过改变TiO2薄膜SiO2薄膜的厚度实现中心波长的调控,进而实现对热电子光电探测器的吸收率光谱和光电响应谱的调节。In the present embodiment, the one-dimensional photonic crystal 6 is formed by periodically alternately arranging uniform dielectric thin films, and the thin film dielectrics are TiO 2 (titanium dioxide) and SiO 2 (silicon dioxide). The arrangement period of the one-dimensional photonic crystal is 5 to 10 periods, and each period includes a layer of TiO2 film and a layer of SiO2 film; the thickness of one layer of TiO2 film is 146nm to 171nm, and the thickness of the one layer of SiO2 film is 146nm to 171nm. The thickness is 218 nm to 253 nm; the thickness of the one-dimensional photonic crystal period is 364 nm to 424 nm. Wherein, the center wavelength of the forbidden band of the one-dimensional photonic crystal in the one-dimensional photonic crystal period can be adjusted by changing the thickness of the TiO 2 film and the SiO 2 film, thereby realizing the absorption rate spectrum of the thermionic photodetector. and modulation of the photoresponse spectrum.

在本实施例中,所述金属连接层4为Ti薄膜,厚度为0.5nm,所述金属层5为Au薄膜,厚度为10nm至35nm。Au薄膜与一维光子晶体之间存在TPP(塔姆等离激化激元)模式,通过改变Au薄膜的厚度,可以实现器件吸收率的优化。In this embodiment, the metal connection layer 4 is a Ti film with a thickness of 0.5 nm, and the metal layer 5 is an Au film with a thickness of 10 nm to 35 nm. There is a TPP (Tam Plasmonic Polarization) mode between the Au thin film and the one-dimensional photonic crystal. By changing the thickness of the Au thin film, the device absorptivity can be optimized.

本实施例的热电子光电探测器器件采用多层平面结构构成,其具体制备过程如下:The thermionic photodetector device of the present embodiment adopts a multi-layer planar structure, and its specific preparation process is as follows:

(1)对双抛Si基底进行清洗,将Si片分别放置在丙酮、无水乙醇中超声清洗15min,随后用去离子水清洗,再用缓冲氧化物刻蚀液清洗30秒以去掉Si表面的氧化层,最后用去离子水清洗并用氮气枪吹干。(1) The double-polished Si substrate was cleaned, and the Si wafers were placed in acetone and absolute ethanol for ultrasonic cleaning for 15 minutes, then cleaned with deionized water, and then cleaned with buffer oxide etching solution for 30 seconds to remove the Si surface. The oxide layer was finally rinsed with deionized water and blown dry with a nitrogen gun.

(2)将Si片的其中一面作为底面,加上掩模板一,采用磁控溅射法制备欧姆接触电极,首先溅射Ti薄膜作为第一电极连接层,再在Ti膜上溅射Au薄膜作为第一电极层。(2) One side of the Si sheet is used as the bottom surface, and a mask plate is added to prepare an ohmic contact electrode by magnetron sputtering. First, a Ti film is sputtered as the first electrode connection layer, and then an Au film is sputtered on the Ti film. as the first electrode layer.

(3)在Si片的另一面上加上掩膜板一,采用电子束蒸发法蒸镀Ti薄膜作为金属连接层,蒸镀Au薄膜作为金属层;Ti层作为Au薄膜与Si基底之间的粘附层,0.5nm的厚度保证Au薄膜和Si基底之间不会形成欧姆接触。(3) A mask plate is added to the other side of the Si sheet, and the Ti film is evaporated by electron beam evaporation as the metal connection layer, and the Au film is evaporated as the metal layer; the Ti layer is used as the connection between the Au film and the Si substrate. The adhesion layer, with a thickness of 0.5 nm, ensures that no ohmic contact is formed between the Au thin film and the Si substrate.

(4)在金属层上加上掩膜板二,采用电子束蒸发法交替蒸镀TiO2薄膜和SiO2薄膜,制得一维光子晶体。掩膜板二覆盖的部位将裸露金属层,在金属层边沿位置制备第二电极。(4) A second mask plate is added on the metal layer, and the TiO 2 film and the SiO 2 film are alternately deposited by electron beam evaporation to obtain a one-dimensional photonic crystal. The part covered by the second mask plate will expose the metal layer, and a second electrode is prepared at the edge of the metal layer.

参见图2,吸收峰波长为1600nm的器件的峰值吸收为51.5%,FWHM为34nm;吸收峰波长为1300nm的器件的峰值为39.1%,FWHM为45nm。Referring to Figure 2, the peak absorption of the device with the absorption peak wavelength of 1600 nm is 51.5%, and the FWHM is 34 nm; the peak absorption of the device with the absorption peak wavelength of 1300 nm is 39.1%, and the FWHM is 45 nm.

选取Tamm耦合中心波长为1500nm的器件结构,当Au薄膜的厚度分别为10nm、15nm、20nm、25nm和35nm时,对比了Au薄膜的厚度对器件最优吸收的差异。The device structure with the Tamm coupling center wavelength of 1500nm was selected. When the thickness of the Au film was 10nm, 15nm, 20nm, 25nm and 35nm, the differences in the optimal absorption of the device by the thickness of the Au film were compared.

参见图3,采用的Au层厚度越厚,光谱带宽也越窄。Au层厚度为35nm的器件的吸收率约为20nm的2倍,FWHM为29nm。Referring to Figure 3, the thicker the thickness of the Au layer used, the narrower the spectral bandwidth. The absorptivity of the device with Au layer thickness of 35 nm is about 2 times that of 20 nm, and the FWHM is 29 nm.

实施例2Example 2

在本实施例中,金属层Au薄膜厚度为30nm;一维光子晶体的排列周期为5个周期,一维光子晶体中的一层TiO2薄膜的厚度为146nm,一层SiO2薄膜的厚度为218nm。In this embodiment, the thickness of the metal layer Au film is 30 nm; the arrangement period of the one-dimensional photonic crystal is 5 periods, the thickness of a layer of TiO 2 film in the one-dimensional photonic crystal is 146 nm, and the thickness of a layer of SiO 2 film is 218nm.

参见图4,在-1V偏压下,器件在1300nm到1500nm波段的光电流响应度达到0.01mA/W到0.1mA/W;在波长为1415nm的峰值响应处,0V偏压下和-1V偏压下分别获得了0.08mA/W和0.1mA/W的光电响应度,FWHM为105nm。Referring to Figure 4, under -1V bias, the photocurrent responsivity of the device in the 1300nm to 1500nm band reaches 0.01mA/W to 0.1mA/W; at the peak response at the wavelength of 1415nm, under 0V bias and -1V bias The photoresponsivity of 0.08 mA/W and 0.1 mA/W were obtained by pressing down, respectively, and the FWHM was 105 nm.

实施例3:Example 3:

在本实施例中,金属层Au薄膜厚度为30nm;一维光子晶体的排列周期为6个周期,一维光子晶体中的一层TiO2薄膜的厚度为171nm,一层SiO2薄膜的厚度为253nm。In this embodiment, the thickness of the metal layer Au film is 30 nm; the arrangement period of the one-dimensional photonic crystal is 6 periods, the thickness of a layer of TiO 2 film in the one-dimensional photonic crystal is 171 nm, and the thickness of a layer of SiO 2 film is 253nm.

参见图5,在-1V偏压下,器件在1505nm到1625nm波段的光电流响应度达到3.56μA/W到13μA/W;在波长为1580nm的峰值响应处,0V偏压下和-1V偏压下分别为10.4μA/W和13μA/W的光电响应度,FWHM为60nm。Referring to Figure 5, under -1V bias, the photocurrent responsivity of the device in the 1505nm to 1625nm band reaches 3.56μA/W to 13μA/W; at the peak response at the wavelength of 1580nm, under 0V bias and -1V bias The lower photoelectric responsivity is 10.4 μA/W and 13 μA/W, respectively, and the FWHM is 60 nm.

上述实施例1、2和3的实验结果说明,基于TPP模式的Si基热电子光电探测器在近红外波段1300nm至1600nm范围工作是可行的,并具有明显的光电响应。The experimental results of the above examples 1, 2 and 3 show that the Si-based thermionic photodetector based on the TPP mode is feasible to work in the near-infrared wavelength range from 1300 nm to 1600 nm, and has obvious photoelectric response.

上述为本实用新型较佳的实施方式,但本实用新型的实施方式并不受上述内容的限制,其他的任何未背离本实用新型的精神实质与原理下所做的改变、修饰、替代、组合、简化,均应为等效的置换方式,都包含在本实用新型的保护范围之内。The above are the preferred embodiments of the present utility model, but the embodiments of the present utility model are not limited by the above-mentioned contents, and any other changes, modifications, substitutions, and combinations made without departing from the spirit and principle of the present utility model , simplification, all should be equivalent replacement methods, and are all included in the protection scope of the present invention.

Claims (10)

1.一种近红外响应的热电子光电探测器,其特征在于,包括自下而上排列的第一电极层薄膜、第一电极连接层薄膜、基底、金属连接层、金属层薄膜和一维光子晶体;所述金属层薄膜上设置有第二电极。1. a thermal electron photodetector of near-infrared response, is characterized in that, comprises the first electrode layer film, the first electrode connection layer film, the substrate, the metal connection layer, the metal layer film and the one-dimensional film arranged from bottom to top A photonic crystal; a second electrode is arranged on the metal layer film. 2.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述一维光子晶体由均匀薄膜介质周期性交替排列而成。2 . The near-infrared responsive thermionic photodetector according to claim 1 , wherein the one-dimensional photonic crystals are formed by periodically alternately arranging uniform thin film media. 3 . 3.根据权利要求2所述的近红外响应的热电子光电探测器,其特征在于,所述一维光子晶体的薄膜介质为TiO2和SiO23 . The near-infrared responsive thermionic photodetector according to claim 2 , wherein the thin film medium of the one-dimensional photonic crystal is TiO 2 and SiO 2 . 4 . 4.根据权利要求2所述的近红外响应的热电子光电探测器,其特征在于,所述一维光子晶体的排列周期为5至10个周期,每一周期包括一层TiO2薄膜和一层SiO2薄膜;所述一维光子晶体的周期的厚度为364nm至424nm。4. The near-infrared responsive thermionic photodetector according to claim 2, wherein the one-dimensional photonic crystal has an arrangement period of 5 to 10 periods, and each period comprises a layer of TiO 2 film and a layer of SiO 2 thin film; the thickness of the period of the one-dimensional photonic crystal is 364 nm to 424 nm. 5.根据权利要求4所述的近红外响应的热电子光电探测器,其特征在于,一层TiO2薄膜的厚度为146nm至171nm;一层SiO2薄膜的厚度为218nm至253nm。5 . The near-infrared response thermionic photodetector according to claim 4 , wherein the thickness of one layer of TiO 2 thin film is 146 nm to 171 nm; the thickness of one layer of SiO 2 thin film is 218 nm to 253 nm. 6 . 6.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述基底为单晶Si晶片。6 . The near-infrared response thermionic photodetector according to claim 1 , wherein the substrate is a single crystal Si wafer. 7 . 7.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述金属连接层为Ti薄膜,厚度为0.5nm。7 . The near-infrared response thermionic photodetector according to claim 1 , wherein the metal connection layer is a Ti film with a thickness of 0.5 nm. 8 . 8.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述金属层为Au薄膜,厚度为10nm至35nm。8 . The near-infrared responsive thermionic photodetector according to claim 1 , wherein the metal layer is an Au thin film with a thickness of 10 nm to 35 nm. 9 . 9.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述第一电极连接层为Ti薄膜,厚度为30nm至50nm。9 . The near-infrared responsive thermionic photodetector according to claim 1 , wherein the first electrode connection layer is a Ti film with a thickness of 30 nm to 50 nm. 10 . 10.根据权利要求1所述的近红外响应的热电子光电探测器,其特征在于,所述第一电极层为Au薄膜,厚度为20nm至100nm。10 . The near-infrared responsive thermionic photodetector according to claim 1 , wherein the first electrode layer is an Au thin film with a thickness of 20 nm to 100 nm. 11 .
CN202123202776.6U 2021-12-17 2021-12-17 Near-infrared response thermal electron photoelectric detector Active CN216488081U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202123202776.6U CN216488081U (en) 2021-12-17 2021-12-17 Near-infrared response thermal electron photoelectric detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202123202776.6U CN216488081U (en) 2021-12-17 2021-12-17 Near-infrared response thermal electron photoelectric detector

Publications (1)

Publication Number Publication Date
CN216488081U true CN216488081U (en) 2022-05-10

Family

ID=81425896

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202123202776.6U Active CN216488081U (en) 2021-12-17 2021-12-17 Near-infrared response thermal electron photoelectric detector

Country Status (1)

Country Link
CN (1) CN216488081U (en)

Similar Documents

Publication Publication Date Title
CN102829884B (en) High-speed SNSPD with strong absorption structure and its preparation method
CN103579405B (en) There is high speed SNSPD of strong absorbing structure and preparation method thereof
CN110098267A (en) A kind of graphene mid-infrared light detector and preparation method thereof based on the enhancing of phonon excimer
CN110224041B (en) A photodetector containing a graphene sandwich structure
CN108630782B (en) Preparation method of wide detection waveband dual-plasma working photoelectric detector
CN110289335A (en) Self-driven near-infrared long-wave photodetector based on In2Se3/Si vertical structure heterojunction and its fabrication method
CN111564504B (en) A solar-blind ultraviolet detector and preparation method thereof
CN111341875A (en) Graphene/palladium diselenide/silicon heterojunction self-driven photoelectric detector
WO2022088204A1 (en) Ultraviolet-visible-near-infrared silicon-based photodetector and production method therefor
CN110752268A (en) Preparation method of MSM photoelectric detector integrated with period light-limiting structure
CN110854234A (en) Graphene photoelectric detector based on interdigital electrode structure
CN113782621A (en) A kind of plasmon enhanced mercury cadmium telluride microcavity infrared detector and preparation method
CN108321242B (en) Optical detector and preparation method thereof based on graphene and coupling grating
CN110137301A (en) Graphene photodetector and preparation method thereof based on metal array structure
CN112201705A (en) Silicon-based ultra-wide spectrum photon absorber and preparation method thereof
CN108807586B (en) A kind of band logical solar blind ultraviolet detector and preparation method thereof polarizing selection characteristic based on gallium oxide
CN108365345B (en) Antenna structure for terahertz microbolometer and preparation method thereof
CN116259676A (en) Novel photoelectric detector and preparation method thereof
CN216488081U (en) Near-infrared response thermal electron photoelectric detector
CN110391314B (en) A narrow-band photoelectric detector and a method for preparing the same
CN118588792A (en) Sandwich graphene quantum dot photoelectric detector and preparation method thereof
CN108281496A (en) A kind of silicon substrate PiN ultraviolet photodiodes and preparation method thereof
CN117650190A (en) Plasmon electrode photoelectric detector suitable for unpolarized light
CN210040233U (en) Narrow spectral response thermionic photoelectric detector
CN113284964B (en) A guided mode photodetector

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant