CN106872052A - A kind of wide spectrum pyroelectric detector absorbing coatings structure and preparation method thereof - Google Patents
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Abstract
本发明公开了一种宽光谱热释电探测器吸收膜系结构及其制备方法,属于热释电探测器红外吸收层领域,解决现有技术中多孔材料与衬底附着性差、且只能单独用作吸收层的问题。该膜系结构制备在热释电探测器敏感单元的顶层,包括三层金属薄膜,底层金属薄膜具有低孔隙率和高致密度,可与衬底保持良好的附着性,中间层金属薄膜作为过渡层,孔隙率提高、致密度降低,顶层金属薄膜为疏松层,可有效增强红外吸收率。所制备的金属吸收层可同时作为吸收层和探测器的上电极,极大简化制备工艺,节约成本,提高工艺兼容性,为高性能热释电探测器的研制提供有力支持。
The invention discloses a wide-spectrum pyroelectric detector absorption film system structure and a preparation method thereof, belonging to the field of infrared absorption layers of pyroelectric detectors, and solves the problem of poor adhesion between porous materials and substrates in the prior art and can only be used alone Problems with being used as an absorbent layer. The film structure is prepared on the top layer of the sensitive unit of the pyroelectric detector, including three layers of metal film, the bottom metal film has low porosity and high density, and can maintain good adhesion with the substrate, and the middle layer of metal film serves as a transition Layer, the porosity is increased, the density is reduced, and the top metal film is a loose layer, which can effectively enhance the infrared absorption rate. The prepared metal absorbing layer can be used as the absorbing layer and the upper electrode of the detector at the same time, which greatly simplifies the preparation process, saves costs, improves process compatibility, and provides strong support for the development of high-performance pyroelectric detectors.
Description
技术领域technical field
本发明涉及热释电探测器红外吸收层技术领域,具体涉及一种宽光谱热释电探测器吸收膜系结构及其制备方法。The invention relates to the technical field of infrared absorbing layers of pyroelectric detectors, in particular to a wide-spectrum pyroelectric detector absorbing film structure and a preparation method thereof.
背景技术Background technique
热释电探测器是一种红外辐射的探测器件,它利用热释电体的自发极化随温度变化的特性制备而成。与其他探测器相比,它不仅保持了热探测器在室温波段工作的优点,而且能承受大的辐射功率、在宽的温度和频率范围内有较高的探测率及具有较小的时间常数等特点。热释电探测器广泛应用于国防、工业、医学和科学研究等领域,例如入侵报警、安全监视、防火报警、工业生产监控、飞机车辆辅助驾驶、医疗诊断等诸多方面。Pyroelectric detector is a kind of infrared radiation detection device, which is prepared by utilizing the characteristic of spontaneous polarization of pyroelectric body changing with temperature. Compared with other detectors, it not only maintains the advantages of thermal detectors working in the room temperature band, but also can withstand large radiation power, have a higher detection rate in a wide temperature and frequency range, and have a smaller time constant Features. Pyroelectric detectors are widely used in the fields of national defense, industry, medicine and scientific research, such as intrusion alarm, security monitoring, fire alarm, industrial production monitoring, aircraft and vehicle auxiliary driving, medical diagnosis and many other aspects.
探测率是衡量热释电探测器性能的主要指标,增大吸收系数是提高探测器探测率的直接途径。研究发现,热释电材料自身在远红外波段具有较高的反射率。尤其在11-20μm波段反射率高达85%(V.Norkus,etc,“A 256pixel pyroelectric linear array withnew black coating”,Proc.of SPIE,vol.8012,pp.80123V,2011)。增加敏感元的厚度可以在一定程度上降低反射率,但是会影响材料热释电系数。为了有效吸收热辐射,进而改善器件的响应率,需要在敏感元表面覆盖一层吸收层或者减反层。要求红外吸收层的反射率低,与底层材料的粘附性要好。The detectability is the main index to measure the performance of the pyroelectric detector, and increasing the absorption coefficient is the direct way to improve the detectability of the detector. Studies have found that pyroelectric materials themselves have high reflectivity in the far-infrared band. Especially in the 11-20μm band, the reflectivity is as high as 85% (V.Norkus, etc, "A 256pixel pyroelectric linear array with new black coating", Proc.of SPIE, vol.8012, pp.80123V, 2011). Increasing the thickness of the sensing element can reduce the reflectivity to a certain extent, but it will affect the pyroelectric coefficient of the material. In order to effectively absorb thermal radiation and improve the responsivity of the device, it is necessary to cover an absorbing layer or an anti-reflection layer on the surface of the sensitive element. It is required that the infrared absorbing layer has low reflectivity and good adhesion to the underlying material.
目前常用的红外辐射吸收层材料主要包括:超薄金属薄膜、有机黑体、多孔型黑金属等。在这几种物质中,超薄金属薄膜反射率也比较低,且热导率较高,但其吸收率的理论极限值较低。黑色树脂的红外吸收率较高,但与器件工艺兼容性差,而且热阻较大,可能会阻碍热量向敏感薄膜的传播。多孔黑金反射率低,具有较高的宽谱吸收特性,但它的粘附性较弱,而且容易破碎。此外,部分文献报道了在敏感材料钽酸锂(LiTaO3)表面刻蚀出折射率渐变型的减反层(A.Finn,etc,“Microstructured surfaces on LiTaO3-basedpyroelectric infrared detectors”,IEEE Sensors Journal,vol.11,pp.2204,2011),基于该减反层结构,吸收率得到明显改善,但该方法对敏感材料表面形貌进行改变,一定程度上影响到器件的响应特性。At present, the commonly used infrared radiation absorbing layer materials mainly include: ultra-thin metal film, organic black body, porous black metal, etc. Among these substances, the ultra-thin metal film has relatively low reflectivity and high thermal conductivity, but the theoretical limit value of its absorptivity is low. Black resin has a high infrared absorption rate, but is poorly compatible with the device process, and has a large thermal resistance, which may hinder the transmission of heat to sensitive films. Porous black gold has low reflectivity and high broad-spectrum absorption characteristics, but it has weak adhesion and is easy to break. In addition, some literatures reported that a graded-index antireflection layer was etched on the surface of the sensitive material lithium tantalate (LiTaO 3 ) (A.Finn, etc., “Microstructured surfaces on LiTaO 3 -based pyroelectric infrared detectors”, IEEE Sensors Journal , vol.11, pp.2204, 2011), based on the anti-reflection layer structure, the absorption rate is significantly improved, but this method changes the surface morphology of sensitive materials, which affects the response characteristics of the device to a certain extent.
发明内容Contents of the invention
本发明所要解决的技术问题为:如何提供一种实现宽光谱红外吸收的膜系结构,该结构能有效增强红外辐射吸收率,为高性能热释电探测器的研制提供有力支持。The technical problem to be solved by the present invention is: how to provide a film structure that realizes wide-spectrum infrared absorption, which can effectively enhance the absorption rate of infrared radiation, and provide strong support for the development of high-performance pyroelectric detectors.
本发明的技术方案为:一种宽光谱热释电探测器吸收膜系结构,该膜系结构位于热释电探测器敏感单元的顶层,该膜系结构包括底层金属薄膜、中间层金属薄膜和顶层金属薄膜,底层金属薄膜、中间层金属薄膜、顶层金属薄膜的孔隙率依次增大。The technical solution of the present invention is: a wide-spectrum pyroelectric detector absorbing film structure, the film structure is located on the top layer of the sensitive unit of the pyroelectric detector, the film structure includes a bottom metal film, a middle layer metal film and The porosity of the top metal film, the bottom metal film, the middle metal film, and the top metal film increases sequentially.
进一步地,底层金属薄膜、中间层金属薄膜和顶层金属薄膜的材料为黑金、铋、铝、钛、镍、铬或者上述金属中的合金。Further, the materials of the bottom metal film, the middle metal film and the top metal film are black gold, bismuth, aluminum, titanium, nickel, chromium or alloys of the above metals.
进一步地,该膜系结构在1~20μm波段红外吸收率优于60%。Further, the infrared absorption rate of the film structure in the 1-20 μm band is better than 60%.
进一步地,底层金属薄膜的孔隙率为15~20%,中间层金属薄膜的孔隙率为30~35%,顶层金属薄膜的孔隙率为45~50%。Further, the porosity of the bottom metal film is 15-20%, the porosity of the middle metal film is 30-35%, and the porosity of the top metal film is 45-50%.
进一步地,底层金属薄膜的厚度为8~12nm,中间层金属薄膜的厚度为10~15nm,顶层金属薄膜的厚度为10~15nm。Further, the thickness of the bottom metal film is 8-12 nm, the thickness of the middle metal film is 10-15 nm, and the thickness of the top metal film is 10-15 nm.
一种宽光谱热释电探测器吸收膜系结构的制备方法,包括以下步骤:A method for preparing a wide-spectrum pyroelectric detector absorbing film structure, comprising the following steps:
(1)在热释电敏感单元的顶层采用磁控溅射法制备致密化的底层金属薄膜;(1) Prepare a densified underlying metal film by magnetron sputtering on the top layer of the pyroelectric sensitive unit;
(2)在步骤(1)所得的致密化的底层金属薄膜上采用磁控溅射法制备较为疏松的中间层金属薄膜;(2) adopt magnetron sputtering method to prepare comparatively loose middle layer metal film on the densified bottom metal film of step (1) gained;
(3)在步骤(2)所得中间层金属薄膜上采用蒸发法或磁控溅射法制备疏松的顶层金属薄膜。(3) Prepare a loose top layer metal film on the middle layer metal film obtained in step (2) by evaporation or magnetron sputtering.
进一步地,步骤(1)的具体步骤为:采用磁控溅射法制备底层金属薄膜,以铋、铝、钛、镍、铬或者它们的合金为材料,工作气压控制在4-6Pa,溅射电流为0.4-0.6A,同时控制薄膜孔隙率范围在15~20%,薄膜厚度范围在8-12nm。Further, the specific steps of step (1) are: using magnetron sputtering to prepare the underlying metal film, using bismuth, aluminum, titanium, nickel, chromium or their alloys as materials, the working pressure is controlled at 4-6Pa, sputtering The electric current is 0.4-0.6A, and at the same time, the porosity of the film is controlled in the range of 15-20%, and the film thickness is in the range of 8-12nm.
进一步地,步骤(2)的具体步骤为:采用磁控溅射法制备中间层金属薄膜,以铋、铝、钛、镍、铬或者它们的合金为材料,工作气压控制在8-10Pa,溅射电流范围为0.2-0.3A,同时控制薄膜孔隙率范围在30~35%,薄膜厚度范围在10-15nm。Further, the specific steps of step (2) are: using magnetron sputtering method to prepare the middle layer metal film, using bismuth, aluminum, titanium, nickel, chromium or their alloys as materials, the working pressure is controlled at 8-10Pa, sputtering The range of the jet current is 0.2-0.3A, and the porosity of the film is controlled at 30-35%, and the film thickness is at 10-15nm.
进一步地,步骤(3)的具体步骤为:采用磁控溅射法制备顶层金属薄膜,以铋、铝、钛、镍、铬或者它们的合金为材料,工艺气压为12-14Pa,溅射电流为0.1A,同时控制薄膜孔隙率范围在45~50%,薄膜厚度范围在10-15nm。Further, the specific steps of step (3) are: using magnetron sputtering to prepare the top metal thin film, using bismuth, aluminum, titanium, nickel, chromium or their alloys as materials, the process pressure is 12-14Pa, the sputtering current 0.1A, while controlling the porosity of the film in the range of 45-50%, and the film thickness in the range of 10-15nm.
进一步地,步骤(3)的具体步骤为:采用蒸发方法制备顶层金属薄膜,以黑金、铋、铝、钛、镍、铬或者它们的合金为材料,调节N2气压为20Pa,控制膜厚低于20nm,形成疏松的多孔状金属层。Further, the specific steps of step (3) are: adopt the evaporation method to prepare the top metal thin film, use black gold, bismuth, aluminum, titanium, nickel, chromium or their alloys as materials, adjust the N pressure to 20Pa , control the film thickness to a low At 20 nm, a loose porous metal layer is formed.
与现有技术相比,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:
本发明的所制备的膜系结构的底层金属薄膜致密度高,与敏感层保持良好的附着性,顶层金属薄膜疏松多孔,有效增强红外吸收率。所制备的金属吸收层可同时作为吸收层和探测器的上电极,极大简化制备工艺,节约成本,提高工艺兼容性,为高性能热释电探测器的研制提供有力支持。The bottom metal thin film of the prepared membrane structure of the present invention has high density and maintains good adhesion with the sensitive layer, and the top layer metal thin film is loose and porous and effectively enhances the infrared absorptivity. The prepared metal absorbing layer can be used as the absorbing layer and the upper electrode of the detector at the same time, which greatly simplifies the preparation process, saves costs, improves process compatibility, and provides strong support for the development of high-performance pyroelectric detectors.
附图说明Description of drawings
图1为本发明的膜系结构的简易制备流程示意图;Fig. 1 is a schematic diagram of a simple preparation process of the film structure of the present invention;
图2为本发明制备的膜系结构的结构示意图;Fig. 2 is the structural representation of the membrane system structure that the present invention prepares;
图中附图标记为,1、热释电敏感单元,2、底层金属薄膜,3、中间层金属薄膜,4、顶层金属薄膜,5、下电极。The reference signs in the figure are: 1. Pyroelectric sensitive unit, 2. Bottom metal film, 3. Middle metal film, 4. Top metal film, 5. Lower electrode.
具体实施方式detailed description
一种宽光谱热释电探测器吸收膜系结构,该膜系结构位于热释电探测器敏感单元的顶层,包括底层金属薄膜、中间层金属薄膜和顶层金属薄膜,底层金属薄膜、中间层金属薄膜、顶层金属薄膜的孔隙率逐渐增大。制备流程如图1所示。A wide-spectrum pyroelectric detector absorbing film structure, the film structure is located on the top layer of the sensitive unit of the pyroelectric detector, including the bottom metal film, the middle layer metal film and the top layer metal film, the bottom metal film, the middle layer metal film The porosity of the film and the top metal film gradually increases. The preparation process is shown in Figure 1.
在衬底上制备的底层金属薄膜要求致密度很高,孔隙率很低,实现吸收层与衬底良好的粘附力。金属材料可以为采用磁控溅射设备制备的铋、铝、钛、镍、铬或者它们的合金薄膜。通过气压和溅射电流调节材料的致密度,气压降低以及电流提高将减弱原子散射效应和提高溅射原子的动能,有利于薄膜微观结构的致密化。因此在制备底层层金属薄膜时,工作气压需控制在4-6Pa,溅射电流为0.4-0.6A。控制孔隙率范围为15~20%,同时控制其膜厚范围在8-12nm,减小对探测器的热容影响。The underlying metal thin film prepared on the substrate requires high density and low porosity to achieve good adhesion between the absorbing layer and the substrate. The metal material can be bismuth, aluminum, titanium, nickel, chromium or their alloy films prepared by magnetron sputtering equipment. The density of the material is adjusted by the gas pressure and the sputtering current. The reduction of the gas pressure and the increase of the current will weaken the atomic scattering effect and increase the kinetic energy of the sputtered atoms, which is beneficial to the densification of the microstructure of the film. Therefore, when preparing the bottom metal thin film, the working pressure should be controlled at 4-6Pa, and the sputtering current should be 0.4-0.6A. The porosity is controlled in the range of 15-20%, and the film thickness is controlled in the range of 8-12nm, so as to reduce the influence on the heat capacity of the detector.
中间层金属薄膜为过渡层,可以适当提高孔隙率和疏松性。该层金属材料可以为采用磁控溅射设备制备的铋、铝、钛、镍、铬或者它们的合金薄膜。通过适当提高气压和降低溅射电流,降低薄膜结构的致密化,控制孔隙率范围为30~35%。工作气压需控制在8-10Pa,溅射电流范围为0.2-0.3A。同时控制其膜厚范围在10-15nm,减小对探测器的热容影响。The metal thin film in the middle layer is a transition layer, which can appropriately increase the porosity and porosity. The metal material of this layer can be bismuth, aluminum, titanium, nickel, chromium or their alloy films prepared by magnetron sputtering equipment. By appropriately increasing the gas pressure and reducing the sputtering current, the densification of the thin film structure is reduced, and the porosity is controlled within a range of 30-35%. The working pressure needs to be controlled at 8-10Pa, and the sputtering current range is 0.2-0.3A. At the same time, the film thickness range is controlled within 10-15nm to reduce the influence on the heat capacity of the detector.
顶层金属薄膜要求疏松多孔,有效增强红外吸收率。金属材料可以为采用磁控溅射设备制备的铋、铝、钛、镍、铬或者它们的合金薄膜。通过在高气压环境中采用Ar等离子溅射,并使用低溅射电流,有效增强原子散射效应及削减原子动能,形成类似黑金的疏松多孔金属层结构,实现红外辐射的宽光谱吸收。控制孔隙率范围为45~50%,同时控制其膜厚范围在10-15nm,减小对探测器的热容影响。顶层层金属吸收层还可以为用蒸发方法制备的黑金、铋、铝、钛、或者合金薄膜,如NiCr。通过在高气压的N2环境中制备的金属薄膜较溅射方法制备的金属薄膜更为疏松,可进一步提高红外吸收率。The top metal film is required to be loose and porous to effectively enhance the infrared absorption rate. The metal material can be bismuth, aluminum, titanium, nickel, chromium or their alloy films prepared by magnetron sputtering equipment. By adopting Ar plasma sputtering in a high-pressure environment and using low sputtering current, the atomic scattering effect is effectively enhanced and the atomic kinetic energy is reduced to form a loose porous metal layer structure similar to black gold to achieve broad-spectrum absorption of infrared radiation. The range of the porosity is controlled to be 45-50%, and the film thickness is controlled to be in the range of 10-15nm, so as to reduce the influence on the heat capacity of the detector. The metal absorption layer on the top layer can also be black gold, bismuth, aluminum, titanium, or an alloy thin film prepared by evaporation, such as NiCr. The metal thin film prepared by the high-pressure N2 environment is more porous than the metal thin film prepared by the sputtering method, which can further improve the infrared absorption rate.
以下通过实施例对本发明做进一步说明:The present invention will be further described below by embodiment:
实施例1Example 1
如图2所示,一种宽光谱热释电探测器吸收膜系结构,包括三层孔隙率逐渐增大的金属薄膜,该结构在以LiTaO3晶体薄片作为热释电敏感单元1的顶层上展开。As shown in Figure 2, a wide-spectrum pyroelectric detector absorbing film structure includes three layers of metal thin films with gradually increasing porosity. Expand.
LiTaO3晶体薄片的前期制备流程为:在LiTaO3晶片上制备下电极5;通过研磨与抛光对LiTaO3晶片4进行减薄形成热释电敏感单元1。The pre-preparation process of LiTaO 3 crystal slices is: preparing the lower electrode 5 on the LiTaO 3 wafer; thinning the LiTaO 3 wafer 4 by grinding and polishing to form the pyroelectric sensitive unit 1 .
清洗LiTaO3晶体薄片,在上表面光刻图形化。采用磁控溅射技术制备底层镍铬合金薄膜作为底层金属薄膜2,调节工艺气压为4Pa,溅射电流为0.6A,得到致密的镍铬金属层,孔隙率范围控制在15%,厚度范围控制在10nm。LiTaO 3 crystal thin slices were cleaned and photolithographically patterned on the upper surface. The underlying nickel-chromium alloy film is prepared by magnetron sputtering technology as the underlying metal film 2, the process pressure is adjusted to 4Pa, the sputtering current is 0.6A, and a dense nickel-chromium metal layer is obtained. The porosity range is controlled at 15%, and the thickness range is controlled. at 10nm.
采用磁控溅射技术制备中间层金属薄膜3,为镍铬合金薄膜,调节工艺气压为8Pa,溅射电流为0.4A,孔隙率范围控制在30%,厚度范围控制在15nm。The metal film 3 in the middle layer is prepared by magnetron sputtering technology, which is a nickel-chromium alloy film. The process pressure is adjusted to 8Pa, the sputtering current is 0.4A, the porosity range is controlled at 30%, and the thickness range is controlled at 15nm.
采用磁控溅射技术制备顶层金属薄膜4,为镍铬合金薄膜,调节工艺气压为12Pa,溅射电流为0.3A,孔隙率范围控制在50%,厚度范围控制在15nm,得到非常疏松的多孔状金属层,然后浮胶清洗。The top metal film 4 is prepared by magnetron sputtering technology, which is a nickel-chromium alloy film. The process pressure is adjusted to 12Pa, the sputtering current is 0.3A, the porosity range is controlled at 50%, and the thickness range is controlled at 15nm to obtain a very loose porous Shaped metal layer, and then floating glue cleaning.
得到宽光谱热释电探测器用红外吸收层,按入射辐射顺序,从上至下依次为疏松多孔镍铬金属层、镍铬金属过渡层及致密型镍铬金属层。The infrared absorbing layer for wide-spectrum pyroelectric detectors is obtained. According to the sequence of incident radiation, from top to bottom, it is a loose porous nickel-chromium metal layer, a nickel-chromium metal transition layer and a dense nickel-chromium metal layer.
实施例2Example 2
如图2所示,一种宽光谱热释电探测器吸收膜系结构,包括三层孔隙率逐渐增大的金属薄膜,该结构在以LiTaO3晶体薄片作为热释电敏感单元1的顶层上展开。As shown in Figure 2, a wide-spectrum pyroelectric detector absorbing film structure includes three layers of metal thin films with gradually increasing porosity. Expand.
LiTaO3晶体薄片的前期制备流程为:在钽酸锂晶片上制备下电极5;通过研磨与抛光对钽酸锂晶片进行减薄,形成热释电敏感单元1。The pre-preparation process of LiTaO 3 crystal flakes is: preparing the lower electrode 5 on the lithium tantalate wafer; thinning the lithium tantalate wafer by grinding and polishing to form the pyroelectric sensitive unit 1 .
清洗LiTaO3晶体薄片,在上表面光刻图形化。采用磁控溅射技术制备底层金属薄膜2,为铋金属薄膜,调节工艺气压为5Pa,溅射电流为0.7A,得到致密的铋金属层,孔隙率范围控制在20%,厚度范围控制在10nm。LiTaO 3 crystal thin slices were cleaned and photolithographically patterned on the upper surface. The underlying metal film 2 is prepared by magnetron sputtering technology, which is a bismuth metal film. The process pressure is adjusted to 5Pa, and the sputtering current is 0.7A to obtain a dense bismuth metal layer. The porosity range is controlled at 20%, and the thickness range is controlled at 10nm. .
采用磁控溅射技术制备中间层金属薄膜3,为铋金属薄膜,调节工艺气压为7Pa,溅射电流为0.5A,孔隙率范围控制在30%,厚度范围控制在15nm。The middle layer metal thin film 3 is prepared by magnetron sputtering technology, which is a bismuth metal thin film. The process pressure is adjusted to 7Pa, the sputtering current is 0.5A, the porosity range is controlled at 30%, and the thickness range is controlled at 15nm.
采用蒸发法制备顶层金属薄膜4,为铋金属薄膜,调节N2气压为20Pa,孔隙率范围控制在45%,控制膜厚低于20nm,形成疏松的多孔状铋金属层,然后浮胶清洗。The top metal thin film 4 is prepared by evaporation method, which is a bismuth metal thin film. The N2 pressure is adjusted to 20Pa, the porosity range is controlled at 45%, and the film thickness is controlled to be less than 20nm to form a loose porous bismuth metal layer, and then the floating glue is cleaned.
得到宽光谱热释电探测器用红外吸收层,按入射辐射顺序,从上至下依次为顶层疏松多孔铋金属薄膜、中间层铋金属薄膜及底层致密型铋金属薄膜。The infrared absorbing layer for wide-spectrum pyroelectric detectors is obtained. According to the order of incident radiation, from top to bottom, the top layer is loose and porous bismuth metal film, the middle layer is bismuth metal film and the bottom layer is dense bismuth metal film.
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