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CN106784115A - Adjustable PIN structural graphene optical detector of fermi level and preparation method thereof - Google Patents

Adjustable PIN structural graphene optical detector of fermi level and preparation method thereof Download PDF

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CN106784115A
CN106784115A CN201710049335.6A CN201710049335A CN106784115A CN 106784115 A CN106784115 A CN 106784115A CN 201710049335 A CN201710049335 A CN 201710049335A CN 106784115 A CN106784115 A CN 106784115A
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CN106784115B (en
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王军
潘锐
李凯
苟君
蒋亚东
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University of Electronic Science and Technology of China
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    • HELECTRICITY
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    • H10F30/00Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
    • H10F30/10Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices being sensitive to infrared radiation, visible or ultraviolet radiation, and having no potential barriers, e.g. photoresistors
    • HELECTRICITY
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    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
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    • HELECTRICITY
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Abstract

The present invention relates to graphene optical detector field, device of the present invention is followed successively by substrate, metal level, insulating barrier, P doped graphenes layer, dielectric layer and N doped graphenes layer from top to bottom, and grid voltage is added in metal level;There is source electrode, drain electrode, first electrode, wherein source electrode and drain electrode are respectively positioned at the both sides of the first graphene layer, and are connected with the first graphene layer on insulating barrier;First electrode and second electrode are connected positioned at the both sides of the second graphene layer, and first electrode with the second graphene layer respectively;P doped graphenes layer, dielectric layer and N doped graphenes layer constitute PIN structural;First graphene layer, source electrode, drain electrode, insulating barrier and metal level constitute a field-effect transistor.The present invention makes the detector that field-effect transistor structure is mutually combined with PIN structural using grapheme material, realizes ultraviolet to the response quickly detection high of infrared broadband.

Description

费米能级可调的PIN结构石墨烯光探测器及其制备方法PIN structure graphene photodetector with tunable Fermi level and its preparation method

技术领域technical field

本发明涉及石墨烯光探测器领域,具体涉及一种费米能级可调的PIN结构石墨烯光探测器及其制备方法。The invention relates to the field of graphene photodetectors, in particular to a PIN-structure graphene photodetector with adjustable Fermi energy level and a preparation method thereof.

背景技术Background technique

石墨烯(Grahpene)是由单层碳原子紧密堆积成二维蜂窝状晶格结构的一种碳质新材料,其具有优异的机械、电学、热学及光学性能,自2004年Novoselov和Geim的团队用机械剥离法制备出室温存在的单层石墨烯以来,其已逐渐成为研究的热点。在目前已知的材料中,石墨烯无疑是最薄的,单层石墨烯厚度仅为 0.3 纳米(一个碳原子厚度),但它也同时是最坚硬的纳米材料。石墨烯可吸收2.3 %的白光,远高于碳的其他同素异形体。石墨烯在常温下即可观察霍尔效应。石墨烯是一种半金属零带隙材料,这使得它可以通过控制栅极来调节石墨烯的传导率,而且能使得它不可能在低于一定限度的条件下关闭,开启禁带的几种方法已经提出并论证。Graphene (Grahpene) is a new carbonaceous material that is tightly packed into a two-dimensional honeycomb lattice structure by a single layer of carbon atoms. It has excellent mechanical, electrical, thermal and optical properties. Since 2004, the team of Novoselov and Geim Since single-layer graphene at room temperature was prepared by mechanical exfoliation, it has gradually become a research hotspot. Graphene is undoubtedly the thinnest known material, with a single layer of graphene only 0.3 nanometers thick (one carbon atom thick), but it is also the hardest nanomaterial. Graphene can absorb 2.3 percent of white light, much higher than other allotropes of carbon. Graphene can observe the Hall effect at room temperature. Graphene is a semi-metallic zero-bandgap material, which makes it possible to adjust the conductivity of graphene by controlling the gate, and it can make it impossible to turn off below a certain limit, and open several kinds of forbidden bands Methods have been proposed and demonstrated.

石墨烯光探测器大致分为金属石墨烯接触式光探测器,等离子体共振型光探测器,量子点石墨烯混合光探测器,石墨烯异质结型光探测器等等。2009年,Fengnian Xia、Thomas Mueller等人利用机械剥离的石墨烯做出了金属石墨烯接触式光探测器,也是第一个石墨烯光电探测器,它的出现引起了广泛的关注。不足是光响应只有0.5mA/W。2010年Echtermeyer研究了不同纳米结构对光电响应的影响,发现改变纳米结构尺寸可以调节不同波长的光吸收,从而基于石墨烯制备出等离子体共振型光探测器,可惜其光响应率并不高。2012年,Gerasimos Konstantatos提出了将量子点和石墨烯混合,从而制备出量子点石墨烯混合光探测器,该器件响应度很高,不过存在暗电流太大、响应速度慢、响应率低等缺点。Graphene photodetectors are roughly divided into metal graphene contact photodetectors, plasmon resonance photodetectors, quantum dot graphene hybrid photodetectors, graphene heterojunction photodetectors, and so on. In 2009, Fengnian Xia, Thomas Mueller and others used mechanically exfoliated graphene to make a metal graphene contact photodetector, which was also the first graphene photodetector, and its appearance attracted widespread attention. The disadvantage is that the light response is only 0.5mA/W. In 2010, Echtermeyer studied the influence of different nanostructures on the photoelectric response, and found that changing the size of the nanostructures can adjust the light absorption of different wavelengths, thus preparing a plasmon resonance photodetector based on graphene, but unfortunately its photoresponse rate is not high. In 2012, Gerasimos Konstantatos proposed mixing quantum dots and graphene to prepare a quantum dot-graphene hybrid photodetector. This device has high responsivity, but has shortcomings such as too large dark current, slow response speed, and low response rate. .

发明内容Contents of the invention

本发明的目的在于针对现有技术的不足,提供一种费米能级可调的PIN结构石墨烯光探测器及其制备方法,该费米能级可调的PIN结构石墨烯光探测器及其制备方法可以解决石墨烯作为光探测器材料对光的吸收率低、响应速度慢的问题。The purpose of the present invention is to address the deficiencies in the prior art, to provide a PIN structure graphene photodetector with adjustable Fermi energy level and its preparation method, the PIN structure graphene photodetector with adjustable Fermi energy level and The preparation method can solve the problems of low light absorption rate and slow response speed of graphene as a photodetector material.

为达到上述要求,本发明采取的技术方案是:提供一种费米能级可调的PIN结构石墨烯光探测器,从下到上依次为衬底、金属层、绝缘层、第一石墨烯层、介质层及第二石墨烯层;绝缘层上具有源极电极、漏极电极及第一电极,其中源极电极和漏极电极均与第一石墨烯层相连接,第一电极与第二石墨烯层相连接;其中第一石墨烯层和第二石墨烯层中任意一个为P掺杂,另一个为N掺杂,第一石墨烯层、介质层及第二石墨烯层构成PIN结构;第一石墨烯层、源极电极、漏极电极、绝缘层及金属层构成一个场效应晶体管。In order to meet the above-mentioned requirements, the technical solution adopted by the present invention is: provide a PIN structure graphene photodetector with adjustable Fermi level, which is followed by substrate, metal layer, insulating layer, first graphene photodetector from bottom to top. layer, dielectric layer and second graphene layer; the insulating layer has a source electrode, a drain electrode and a first electrode, wherein the source electrode and the drain electrode are all connected to the first graphene layer, and the first electrode is connected to the second graphene layer. Two graphene layers are connected; any one of the first graphene layer and the second graphene layer is P-doped, and the other is N-doped, and the first graphene layer, the dielectric layer and the second graphene layer constitute a PIN Structure; the first graphene layer, the source electrode, the drain electrode, the insulating layer and the metal layer form a field effect transistor.

提供一种费米能级可调的PIN结构石墨烯光探测器的制备方法,包括以下步骤:A method for preparing a PIN structure graphene photodetector with adjustable Fermi level is provided, comprising the following steps:

S1、在衬底表面沉积金属层;S1, depositing a metal layer on the surface of the substrate;

S2、在金属层表面生长绝缘层;S2, growing an insulating layer on the surface of the metal layer;

S3、在绝缘层表面沉积一层金属电极层,光刻金属电极层形成源极电极、漏极电极、第一电极及第二电极;S3. Depositing a metal electrode layer on the surface of the insulating layer, and photoetching the metal electrode layer to form a source electrode, a drain electrode, a first electrode and a second electrode;

S4、转移一层石墨烯至绝缘层表面形成第一石墨烯层,第一石墨烯层分别与源极电极和漏极电极相连接,并对第一石墨烯层进行掺杂;S4, transferring a layer of graphene to the surface of the insulating layer to form a first graphene layer, the first graphene layer is respectively connected to the source electrode and the drain electrode, and the first graphene layer is doped;

S5、在第一石墨烯层表面生长介质层;S5, growing a dielectric layer on the surface of the first graphene layer;

S6、转移一层石墨烯至介质层表面形成第二石墨烯层,第二石墨烯层与第一电极相连接,并对第二石墨烯层进行掺杂;S6. Transferring a layer of graphene to the surface of the dielectric layer to form a second graphene layer, the second graphene layer is connected to the first electrode, and doping the second graphene layer;

S7、刻蚀掉器件表面多余的石墨烯,完成器件的制备S7. Etching away excess graphene on the surface of the device to complete the preparation of the device

该费米能级可调的PIN结构石墨烯光探测器及其制备方法具有的优点如下:The PIN structure graphene photodetector with adjustable Fermi level and the preparation method thereof have the following advantages:

(1)在石墨烯异质结的基础上,在P掺杂石墨烯和N掺杂石墨烯中间加入一层介质层作I层,形成PIN型结构,可以有效降低器件的暗电流,提高器件信噪比,提高本器件作为石墨烯光探测器的响应率和响应速度;(1) On the basis of graphene heterojunction, a dielectric layer is added between P-doped graphene and N-doped graphene as I layer to form a PIN structure, which can effectively reduce the dark current of the device and improve the performance of the device. The signal-to-noise ratio improves the responsivity and response speed of the device as a graphene photodetector;

(2)金属层和绝缘层形成一个谐振腔,使光在腔内不断反射,从而起到提高光响应率的目的,而且谐振腔高度的不同对应着不同的吸收波长;(2) The metal layer and the insulating layer form a resonant cavity, so that the light is continuously reflected in the cavity, so as to improve the light responsivity, and the difference in the height of the resonant cavity corresponds to different absorption wavelengths;

(3)第一石墨烯层、源极电极、漏极电极、绝缘层及金属层构成一个场效应晶体管,通过在金属层上加栅极电压可以调节第一石墨烯层的费米能级,从而得到第一石墨烯层和第二石墨烯层之间变化的费米能级差,有效增强对不同探测波段的响应率。(3) The first graphene layer, the source electrode, the drain electrode, the insulating layer and the metal layer constitute a field effect transistor, and the Fermi level of the first graphene layer can be adjusted by applying a gate voltage to the metal layer, Thus, the changing Fermi level difference between the first graphene layer and the second graphene layer is obtained, which effectively enhances the responsivity to different detection bands.

附图说明Description of drawings

此处所说明的附图用来提供对本申请的进一步理解,构成本申请的一部分,在这些附图中使用相同的参考标号来表示相同或相似的部分,本申请的示意性实施例及其说明用于解释本申请,并不构成对本申请的不当限定。在附图中:The accompanying drawings described here are used to provide a further understanding of the application and constitute a part of the application. In these drawings, the same reference numerals are used to indicate the same or similar parts. The illustrative embodiments of the application and their descriptions are used The purpose of explaining this application does not constitute an improper limitation of this application. In the attached picture:

图1为本申请器件的剖面示意图;Fig. 1 is a schematic cross-sectional view of the device of the present application;

图2为本申请器件的平面示意图;Fig. 2 is the schematic plan view of the device of the present application;

图3为本申请方法的流程示意图;Fig. 3 is a schematic flow chart of the method of the present application;

图4为用SCS4200半导体测试仪测试的器件在632nm的光照变化下的电流变化图。Fig. 4 is a diagram of the current change of the device tested with the SCS4200 semiconductor tester under the light change of 632nm.

具体实施方式detailed description

为使本申请的目的、技术方案和优点更加清楚,以下结合附图及具体实施例,对本申请作进一步地详细说明。In order to make the purpose, technical solution and advantages of the present application clearer, the present application will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.

为简单起见,以下描述中省略了本领域技术人员公知的某些技术特征。For simplicity, some technical features known to those skilled in the art are omitted from the following description.

根据本申请的一个实施例,提供一种费米能级可调的PIN结构石墨烯光探测器,如图1、2所示,从下到上依次为衬底1、金属层2、绝缘层3、第一石墨烯层5、介质层6及第二石墨烯层7,使用时在金属层2加上栅极电压;绝缘层3上具有源极电极4a、漏极电极4b及第一电极4c,一般一次性可以完成4个电极的制作,除了源极电极4a、漏极电极4b和第一电极4c之外的第二电极4d,作为备用电极;其中源极电极4a和漏极电极4b分别位于第一石墨烯层5的两侧,且均与第一石墨烯层5相连接;第一电极4c和第二电极4d分别位于第二石墨烯层7的两侧,且第一电极4c与第二石墨烯层7相连接;其中第一石墨烯层5为P掺杂,第二石墨烯层7为N掺杂,第一石墨烯层5、介质层6及第二石墨烯层7构成PIN结构;第一石墨烯层5、源极电极4a、漏极电极4b、绝缘层3及金属层2构成一个场效应晶体管。According to one embodiment of the present application, a PIN structure graphene photodetector with adjustable Fermi level is provided, as shown in Figures 1 and 2, substrate 1, metal layer 2, insulating layer from bottom to top 3. The first graphene layer 5, the dielectric layer 6 and the second graphene layer 7, when in use, apply a gate voltage to the metal layer 2; the insulating layer 3 has a source electrode 4a, a drain electrode 4b and a first electrode 4c, in general, the production of four electrodes can be completed at one time, and the second electrode 4d other than the source electrode 4a, the drain electrode 4b and the first electrode 4c is used as a spare electrode; wherein the source electrode 4a and the drain electrode 4b Respectively located on both sides of the first graphene layer 5, and all connected with the first graphene layer 5; the first electrode 4c and the second electrode 4d are respectively located on both sides of the second graphene layer 7, and the first electrode 4c Connected with the second graphene layer 7; wherein the first graphene layer 5 is P-doped, the second graphene layer 7 is N-doped, the first graphene layer 5, the dielectric layer 6 and the second graphene layer 7 A PIN structure is formed; the first graphene layer 5, the source electrode 4a, the drain electrode 4b, the insulating layer 3 and the metal layer 2 form a field effect transistor.

进一步的,金属层2为Cu、Au、Al、Ni、NiCr或Ag,且金属层2的厚度为100-1000 nm。Further, the metal layer 2 is Cu, Au, Al, Ni, NiCr or Ag, and the thickness of the metal layer 2 is 100-1000 nm.

进一步的,绝缘层3为SiO2、Si3N4、MnO2或MgO,绝缘层3的厚度为100-1000 nm。Further, the insulating layer 3 is SiO 2 , Si 3 N 4 , MnO 2 or MgO, and the thickness of the insulating layer 3 is 100-1000 nm.

进一步的,介质层6为Si3N4 、MgO、SiO2或未掺杂的石墨烯,介质层6的厚度为1-500nm。Further, the dielectric layer 6 is Si 3 N 4 , MgO, SiO 2 or undoped graphene, and the thickness of the dielectric layer 6 is 1-500 nm.

一种费米能级可调的PIN结构石墨烯光探测器的制备方法,如图3所示,包括以下步骤:A preparation method of a PIN structure graphene photodetector with adjustable Fermi level, as shown in Figure 3, comprises the following steps:

S1、清洗高掺杂的硅衬底1并吹干,在硅衬底1表面沉积一层300nm厚的Cu薄膜作为场效应晶体管栅极及整个器件的金属层2;S1, cleaning the highly doped silicon substrate 1 and blowing it dry, depositing a 300nm thick Cu thin film on the surface of the silicon substrate 1 as the gate of the field effect transistor and the metal layer 2 of the entire device;

S2、以金属层2为基底,用PECVD的方法在上面生长一层300nm厚的SiO2作为场效应晶体管的绝缘层3;S2, with the metal layer 2 as the base, grow a layer of 300nm thick SiO 2 as the insulating layer 3 of the field effect transistor with the method of PECVD;

S3、在绝缘层3表面沉积一层金属电极层,光刻金属电极层形成源极电极4a、漏极电极4b、第一电极4c及第二电极4d;S3, depositing a metal electrode layer on the surface of the insulating layer 3, and photoetching the metal electrode layer to form a source electrode 4a, a drain electrode 4b, a first electrode 4c, and a second electrode 4d;

S4、转移一层石墨烯至绝缘层表面形成第一石墨烯层5,第一石墨烯层5分别与源极电极4a和漏极电极4b相连接,并用旋涂Au和甲苯混合溶液的方法对第一石墨烯层5进行P型掺杂;S4, transfer one layer of graphene to the surface of the insulating layer to form the first graphene layer 5, the first graphene layer 5 is connected with the source electrode 4a and the drain electrode 4b respectively, and the method for spin-coating Au and toluene mixed solution P-type doping is performed on the first graphene layer 5;

S5、在第一石墨烯层5表面生长介质层6;S5, growing a dielectric layer 6 on the surface of the first graphene layer 5;

S6、转移一层石墨烯至介质层表面形成第二石墨烯层7,第二石墨烯层7与第一电极4c相连接,并采用滴涂联氨溶液或旋涂PEI溶液的方法对第二石墨烯层7进行N型掺杂;S6, transfer one layer of graphene to the surface of the medium layer to form the second graphene layer 7, the second graphene layer 7 is connected to the first electrode 4c, and adopt the method of drip coating hydrazine solution or spin coating PEI solution to the second The graphene layer 7 is N-type doped;

S7、刻蚀掉器件表面多余的石墨烯,完成器件的制备。S7. Etching off excess graphene on the surface of the device to complete the preparation of the device.

采用632nm 激光器作为光源进行探测器性能测试。设置栅极电压为-1V,源极与漏极(接地)之间电压为0.5V,采用S[1] 半导体测试仪测试漏极电极4b与第一电极4c之间的电学输出信号,测试结果如图4所示。可以看出该结构探测器在632nm光源斩波后照射下有显著的电学响应信号输出,响应电流约10μA,响应速度低于1ms,通过调节衬底栅极电压可以调节器件的响应电流大小和器件响应的优化波段。因此通过本发明中场效应晶体管与PIN结构相复合的探测器结构获得了高响应率、高响应速度的性能。A 632nm laser was used as the light source for detector performance testing. Set the gate voltage to -1V, the voltage between the source and the drain (ground) to 0.5V, use the S[1] semiconductor tester to test the electrical output signal between the drain electrode 4b and the first electrode 4c, and the test results As shown in Figure 4. It can be seen that the structure of the detector has a significant electrical response signal output under the irradiation of a 632nm light source after chopping, the response current is about 10μA, and the response speed is lower than 1ms. The response current of the device and the The optimized band for the response. Therefore, the performance of high responsivity and high response speed is obtained through the composite detector structure of the field effect transistor and the PIN structure of the present invention.

以上所述实施例仅表示本发明的几种实施方式,其描述较为具体和详细,但并不能理解为对本发明范围的限制。应当指出的是,对于本领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干变形和改进,这些都属于本发明保护范围。因此本发明的保护范围应该以所述权利要求为准。The above-mentioned embodiments only represent several implementations of the present invention, and the description thereof is relatively specific and detailed, but should not be construed as limiting the scope of the present invention. It should be noted that those skilled in the art can make several modifications and improvements without departing from the concept of the present invention, and these all belong to the protection scope of the present invention. Therefore, the protection scope of the present invention should be determined by the claims.

原交底书中记载的是“SCS4200”,请确认。"SCS4200" is recorded in the original submission, please confirm.

Claims (10)

1. the adjustable PIN structural graphene optical detector of a kind of fermi level, it is characterised in that be followed successively by from top to bottom substrate, Metal level, insulating barrier, the first graphene layer, dielectric layer and the second graphene layer;There is source electrode, drain electrode on insulating barrier And first electrode, wherein source electrode and drain electrode be connected with the first graphene layer, first electrode and the second Graphene Layer is connected;Any one is P doping in wherein the first graphene layer and the second graphene layer, and another is that N adulterates, the first stone Black alkene layer, dielectric layer and the second graphene layer constitute PIN structural;First graphene layer, source electrode, drain electrode, insulating barrier And metal level constitutes a field-effect transistor.
2. the adjustable PIN structural graphene optical detector of fermi level according to claim 1, it is characterised in that described Metal level is Cu, Au, Al, Ni, NiCr or Ag, and the thickness of metal level is 100-1000 nm.
3. the adjustable PIN structural graphene optical detector of fermi level according to claim 1, it is characterised in that described Insulating barrier is SiO2、Si3N4、MnO2Or MgO, the thickness of insulating barrier is 100-1000 nm.
4. the adjustable PIN structural graphene optical detector of fermi level according to claim 1, it is characterised in that described Dielectric layer is Si3N4 、MgO、SiO2Or the Graphene of undoped p.
5. the adjustable PIN structural graphene optical detector of fermi level according to claim 1 or 4, it is characterised in that institute The thickness for stating dielectric layer is 1-500 nm.
6. the adjustable PIN structural graphene optical detector of fermi level according to claim 1, it is characterised in that described Also have as standby second electrode on insulating barrier.
7. the preparation method of the adjustable PIN structural graphene optical detector of a kind of fermi level, it is characterised in that including following step Suddenly:
S1, substrate surface deposited metal layer;
S2, layer on surface of metal grow insulating barrier;
S3, layer of metal electrode layer is deposited in surface of insulating layer, photolithographic electrode layer forms source electrode, drain electrode, the One electrode and second electrode;
S4, transfer one layer graphene to surface of insulating layer formed the first graphene layer, the first graphene layer respectively with source electrode It is connected with drain electrode, and the first graphene layer is doped;
S5, in the first graphene layer superficial growth dielectric layer;
S6, one layer graphene of transfer to dielectric layer surface form the second graphene layer, and the second graphene layer is connected with first electrode Connect, and the second graphene layer is doped;
S7, the unnecessary Graphene of device surface is etched away, complete the preparation of device.
8. the preparation method of the adjustable PIN structural graphene optical detector of fermi level according to claim 7, its feature It is that p-type doping is carried out to the first graphene layer in the step S4, n-type doping is carried out to the second graphene layer in step S6; Or n-type doping is carried out to the first graphene layer in step S4, p-type doping is carried out to the second graphene layer in step S6.
9. the preparation method of the adjustable PIN structural graphene optical detector of fermi level according to claim 8, its feature It is that the p-type doping is doped using the method for spin coating Au and toluene mixed solution to graphene layer.
10. the preparation method of the adjustable PIN structural graphene optical detector of fermi level according to claim 8, it is special Levy and be, the n-type doping is doped using the method for drop coating hydrazine solution or spin coating PEI solution to graphene layer.
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