CN1330005C - Ultraviolet reinforced photo detector employing gallium arsenide base phosphorated material and making method - Google Patents

Ultraviolet reinforced photo detector employing gallium arsenide base phosphorated material and making method Download PDF

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CN1330005C
CN1330005C CNB2005100231736A CN200510023173A CN1330005C CN 1330005 C CN1330005 C CN 1330005C CN B2005100231736 A CNB2005100231736 A CN B2005100231736A CN 200510023173 A CN200510023173 A CN 200510023173A CN 1330005 C CN1330005 C CN 1330005C
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gallium arsenide
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phosphorus
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CN1632957A (en
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张永刚
刘天东
李爱珍
齐鸣
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Shanghai Institute of Microsystem and Information Technology of CAS
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Abstract

本发明涉及基于砷化镓基含磷化合物半导体材料的紫外增强光电探测器及制作方法,其特征在于以半绝缘砷化镓单晶材料作为探测器的衬底,在其上采用外延方法生长特定的宽禁带含磷化合物薄膜材料作为有源光吸收层和窗口层,以达到紫外增强光吸收效果并消除其对红外光的响应,并采用合适的掺杂方式在其中构成PN结。外延材料采用特定的选择刻蚀工艺制作出台面结构,经钝化保护后制作出接触电极,并选用相应的抗反射增透膜进一步提高其短波响应。此种光电探测器可应用于火焰探测、紫外和可见光波段光度测量、尾焰跟踪、生物及化学气体检测、紫外线防护等方面,并可与红外波段的光电探测器进行单片或混合集成构成双色探测器。

Figure 200510023173

The invention relates to an ultraviolet-enhanced photodetector based on gallium arsenide-based phosphorus-containing compound semiconductor materials and a manufacturing method, which is characterized in that a semi-insulating gallium arsenide single crystal material is used as the substrate of the detector, and a specific detector is grown on it by an epitaxial method. The wide bandgap phosphorus-containing compound thin film material is used as the active light absorption layer and window layer to achieve the effect of ultraviolet enhanced light absorption and eliminate its response to infrared light, and a PN junction is formed in it by a suitable doping method. The epitaxial material uses a specific selective etching process to produce a mesa structure, and after passivation protection, the contact electrode is produced, and the corresponding anti-reflection and anti-reflection coating is selected to further improve its short-wave response. This kind of photodetector can be used in flame detection, photometric measurement in ultraviolet and visible light bands, tail flame tracking, biological and chemical gas detection, ultraviolet protection, etc., and can be monolithic or mixed with infrared photodetectors to form a two-color detector.

Figure 200510023173

Description

采用砷化镓基含磷材料的紫外增强光电探测器及制作方法Ultraviolet-enhanced photodetector using gallium arsenide-based phosphorus-containing material and manufacturing method

技术领域technical field

本发明涉及采用镓基含磷化合物半导体材料的紫外增强光电探测器及制作方法,更确切地说,本发明提供一种新型光电探测器,它能使光电探测器具有良好的紫外至可见光波段响应,同时充分抑制红外光响应。本发明属于半导体光电子材料与器件技术领域。The invention relates to an ultraviolet-enhanced photodetector using a gallium-based phosphorus-containing compound semiconductor material and a manufacturing method. More precisely, the invention provides a new type of photodetector, which can make the photodetector have a good response in the ultraviolet to visible light band , while sufficiently suppressing the infrared light response. The invention belongs to the technical field of semiconductor optoelectronic materials and devices.

背景技术Background technique

半导体光电探测器作为一种典型的光电器件在众多场合都得到了广泛应用,其工作波段已从可见至近红外波段扩展至中红外乃至远红外波段。硅光电二极管作为一种最常用的光电探测器,在可见光至近红外波段(λ<1.1μm)具有良好的表现,采用一些特殊的工艺技术也可以使其响应波长扩展至紫外波段,但由于探测器工作原理和材料特性的限制,其对长波方向的响应要明显大于短波响应。对一些较特殊的应用而言,人们常需要探测器在短波方向有较高的响应而抑制其在长波方向的响应以避免干扰等,对硅光电探测器而言这就需要采用较复杂的滤光结构,并以牺牲一定的短波响应和增加成本为代价,系统的整体性能也会受到很大限制。自上世纪六十年代各种新型材料特别是半导体材料获得广泛应用以来,基于半导体材料的光电器件已有了长足的发展,材料生长技术也不断进步,具有精确控制能力、适用于生长复杂结构的分子束外延(MBE)和金属有机物气相外延(MOVPE)等生长技术已开始广泛应用,各种商品化的生长设备也已推向市场,使得人们有可能采用新的材料体系来满足不同的要求。本发明人通过选择新的材料体系,提供一种满足前述要求的新型光电探测器。As a typical optoelectronic device, semiconductor photodetectors have been widely used in many occasions, and their operating bands have been extended from visible to near-infrared to mid-infrared and even far-infrared. As one of the most commonly used photodetectors, silicon photodiodes have good performance in the visible light to near-infrared band (λ<1.1 μm). Some special process technologies can also extend the response wavelength to the ultraviolet band. However, due to the Due to the limitations of the working principle and material properties, the response to the long-wave direction is significantly greater than the short-wave response. For some special applications, it is often required that the detector has a higher response in the short-wave direction and suppress its response in the long-wave direction to avoid interference, etc. For silicon photodetectors, this requires a more complex filter. Optical structure, at the cost of sacrificing a certain short-wave response and increasing costs, the overall performance of the system will also be greatly limited. Since various new materials, especially semiconductor materials, were widely used in the 1960s, optoelectronic devices based on semiconductor materials have made great progress, and material growth technology has also continued to improve. They have precise control capabilities and are suitable for growing complex structures. Growth technologies such as molecular beam epitaxy (MBE) and metal organic vapor phase epitaxy (MOVPE) have begun to be widely used, and various commercial growth equipment have also been introduced to the market, making it possible to use new material systems to meet different requirements. The present inventors provide a novel photodetector that meets the aforementioned requirements by selecting a new material system.

发明内容Contents of the invention

本发明的目的在于提供一种采用砷化镓基含磷材料的紫外增强光电探测器及制作方法,也即提供一种新制作的紫外增强光电探测器,利用材料的固有特性完全消除其对红外光响应。并使得探测器具有高量子效率、快响应速度以及高可靠性和抗辐照能力。此种光电探测器可应用于火焰探测、紫外和可见光波段光度测量、尾焰跟踪、生物及化学气体检测、紫外线防护等方面,并可与红外光电探测器集成构成双色探测器等用于特殊场合。本发明的工作原理及其实施是普适的,The purpose of the present invention is to provide an ultraviolet enhanced photodetector using gallium arsenide-based phosphorus-containing materials and a manufacturing method, that is, to provide a newly fabricated ultraviolet enhanced photodetector, which completely eliminates its infrared radiation by using the inherent characteristics of the material. light response. And the detector has high quantum efficiency, fast response speed, high reliability and radiation resistance. This kind of photodetector can be used in flame detection, photometric measurement in ultraviolet and visible light bands, tail flame tracking, biological and chemical gas detection, ultraviolet protection, etc., and can be integrated with infrared photodetectors to form a two-color detector for special occasions . The working principle of the present invention and its implementation are universal,

根据以上技术背景存在的问题和现实的本发明确定了探测器的材料体系并开发了相应的材料生长工艺。半导体光电探测器(量子探测器类)在长波方向上的截止波长是由探测器有源区材料的带隙确定的,为消除探测器对红外光的响应,本发明选取与砷化镓衬底晶格匹配的含磷宽禁带材料体系作为探测器的有源区材料。采用砷化镓作为衬底材料成本相对较低,材料也较成熟质量和供应都有保证。对制作双色探测器等应用而言,本发明选用不掺杂的半绝缘砷化镓材料作为衬底,在其上采用外延生长的宽禁带含磷化合物薄膜作为有源光吸收层和窗口层,并在吸收层和窗口层之间构成PN结,且探测器采用单面电极引出,这样一方面衬底对红外光是透明的(λ>870nm直至中、远红外波段),在集成时可以不影响下探测器的性能,另一方面对短波长(λ<870nm)的光又是不透明的,可以对下探测器起到很好的短波截止滤光片作用,充分抑制下探测器对短波长(λ<870nm)光的响应,这样在很多场合下就不需另加滤光片了。采用砷化镓衬底的另一优点是可以与量子阱红外探测器进行单片集成构成单片型的双色或多色探测器,对于一般应用也可采用高掺杂的N型导电衬底,这时探测器可采用双面电极结构。According to the problems existing in the above technical background and reality, the present invention determines the material system of the detector and develops a corresponding material growth process. The cut-off wavelength of semiconductor photodetectors (quantum detectors) in the long-wave direction is determined by the bandgap of the material in the active region of the detector. In order to eliminate the response of the detector to infrared light, the present invention selects a substrate with GaAs The lattice-matched phosphorus-containing wide-bandgap material system is used as the active region material of the detector. The cost of using gallium arsenide as the substrate material is relatively low, and the material is relatively mature, quality and supply are guaranteed. For applications such as the production of two-color detectors, the present invention selects undoped semi-insulating gallium arsenide material as the substrate, and uses epitaxially grown wide-bandgap phosphorus-containing compound films on it as the active light absorption layer and window layer , and a PN junction is formed between the absorption layer and the window layer, and the detector is led out by a single-sided electrode, so that the substrate is transparent to infrared light (λ>870nm to the mid- and far-infrared band), and can be integrated during integration. It does not affect the performance of the lower detector. On the other hand, it is opaque to short-wavelength (λ<870nm) light, and can play a good role as a short-wave cut-off filter for the lower detector, fully suppressing the short The wavelength (λ<870nm) light response, so in many occasions do not need additional filters. Another advantage of using gallium arsenide substrate is that it can be monolithically integrated with the quantum well infrared detector to form a monolithic two-color or multi-color detector. For general applications, a highly doped N-type conductive substrate can also be used. At this time, the detector can adopt a double-sided electrode structure.

与砷化镓衬底晶格匹配的含磷宽禁带材料体系包括三元系的Ga0.51In0.49P、Al0.52In0.48P和四元系的(AlzGa1-z)0.51In0.49P等,Ga0.51In0.49P为直接带隙材料,室温下的带隙为1.85eV,(AlzGa1-z)0.51In0.49P在0<z<0.55时也为直接带隙材料,其带隙随z增加在1.85-2.26eV之间可调,对应的截止波长可在670-550nm之间变化,Al0.52In0.48P为间接带隙材料,其带隙为2.34eV,因此可以根据探测器截止波长的不同需要对Al和Ga的相对组份进行裁剪。在此材料体系上选取不同组分的材料分别作为光吸收层和窗口层,一种方案是采用带隙相对较小的三元系GaInP作为光吸收层,带隙较大的三元系AlInP作为窗口层,以达到高量子效率和低暗电流的性能,并利用AlInP低折射率的特点,控制窗口层的厚度,使其起到一定的增透和增强短波响应的效果。采用宽禁带材料后可使探测器在光照下的输出电压有大幅度提高,短波响应也可明显改善。此材料体系还具有优良的抗辐照性能。探测器采用分子束外延(MBE)或金属有机物气相外延(MOVPE)方法生长外延材料,并在生长有源光吸收层和窗口层时进行掺杂控制以生长出具有不同导电类型的低掺杂和高掺杂区并形成PN结,我们在生长工艺中选取了较薄的高掺杂层厚度以保证探测器的高响应度和良好的短波响应。此紫外增强光电探测器可采用以下外延结构:半绝缘砷化镓材料(或硅掺杂低阻砷化镓材料)为衬底,首先在其上生长一层n型高掺杂(n>5×1017cm-3)的下接触层(此接触层可为掺硅砷化镓材料,它同时也作为外延缓冲层),然后在其上生长低掺杂或非故意掺杂(n<5×1017cm-3)的含磷宽禁带光吸收层,再在其上生长铍p型高掺杂(p>5×1017cm-3)的含磷宽禁带光吸收层(也可同时包括窗口层),最后生长一层p型高掺杂(p>5×1017cm-3)的上接触层(此接触层可为掺铍砷化镓材料)。Phosphorus-containing wide-bandgap material systems that match the lattice of GaAs substrates include ternary Ga 0.51 In 0.49 P, Al 0.52 In 0.48 P and quaternary (Al z Ga 1-z ) 0.51 In 0.49 P etc., Ga 0.51 In 0.49 P is a direct band gap material, the band gap at room temperature is 1.85eV, (Al z Ga 1-z ) 0.51 In 0.49 P is also a direct band gap material when 0<z<0.55, its band gap The gap is adjustable between 1.85-2.26eV with the increase of z, and the corresponding cut-off wavelength can be changed between 670-550nm. Al 0.52 In 0.48 P is an indirect bandgap material, and its bandgap is 2.34eV, so it can be adjusted according to the detector The difference in cutoff wavelength requires tailoring of the relative compositions of Al and Ga. In this material system, materials with different components are selected as the light absorbing layer and the window layer respectively. One solution is to use the ternary system GaInP with a relatively small band gap as the light absorbing layer, and the ternary system AlInP with a large band gap as the light absorbing layer. The window layer is used to achieve high quantum efficiency and low dark current performance, and the low refractive index of AlInP is used to control the thickness of the window layer to achieve a certain effect of anti-reflection and enhanced short-wave response. The use of wide-bandgap materials can greatly increase the output voltage of the detector under illumination, and the short-wave response can also be significantly improved. This material system also has excellent radiation resistance. The detector uses molecular beam epitaxy (MBE) or metal organic vapor phase epitaxy (MOVPE) to grow epitaxial materials, and controls the doping when growing the active light absorbing layer and window layer to grow low-doped and The highly doped region forms a PN junction. We selected a thinner highly doped layer thickness in the growth process to ensure the high responsivity and good short-wave response of the detector. This UV-enhanced photodetector can adopt the following epitaxial structure: semi-insulating gallium arsenide material (or silicon-doped low-resistance gallium arsenide material) is used as the substrate, and a layer of n-type highly doped (n>5 ×10 17 cm -3 ) lower contact layer (this contact layer can be silicon-doped gallium arsenide material, which also serves as an epitaxial buffer layer), and then grow low-doped or unintentionally doped (n<5 × 10 17 cm -3 ) phosphorus-containing wide-bandgap light - absorbing layer, and then grow a phosphorous-containing wide-bandgap light-absorbing layer (also A window layer may be included at the same time), and finally grow a p-type highly doped (p>5×10 17 cm -3 ) upper contact layer (this contact layer may be beryllium-doped gallium arsenide material).

在生长出高质量的探测器材料的基础上本发明开发了探测器制作工艺及选择刻蚀工艺。探测器制作工艺中我们采用了特殊的选择刻蚀配方,由于器件结构中上下接触层均为不含磷的低阻GaAs材料,本发明利用了接触层非含磷材料及有源光吸收层和窗口层含磷材料的不同化学特性,利用湿法选择腐蚀工艺刻蚀出探测器的台面结构,并在其后制作出自对准的透光窗口,实际工艺中我们利用酒石酸系的腐蚀液(如酒石酸/双氧水体系)刻蚀GaAs材料,当遇到含磷化合物材料时刻蚀会自动停止,利用盐酸系的腐蚀液(如盐酸/磷酸体系)刻蚀含磷化合物,遇到不含磷材料时刻蚀也会自动停止,大大方便了工艺控制。所述酒石酸/双氧水体系是由酒石酸和水以1∶1体积比稀释后再加入5vol%的双氧水组成;盐酸/磷酸的体积比为1∶4,使用的盐酸等为化学纯或分析纯。On the basis of growing high-quality detector materials, the invention develops a detector manufacturing process and a selective etching process. In the detector manufacturing process, we have adopted a special selective etching formula. Since the upper and lower contact layers in the device structure are low-resistance GaAs materials that do not contain phosphorus, the present invention utilizes the non-phosphorus-containing material of the contact layer and the active light absorption layer and According to the different chemical characteristics of the phosphorus-containing materials in the window layer, the mesa structure of the detector is etched by a wet selective etching process, and then a self-aligned light-transmitting window is produced. In the actual process, we use a tartaric acid-based etching solution (such as tartaric acid/hydrogen peroxide system) to etch GaAs materials, when it encounters phosphorus-containing compound materials, the etching will automatically stop, use hydrochloric acid-based etching solution (such as hydrochloric acid/phosphoric acid system) to etch phosphorus-containing compounds, and when encountering phosphorus-free materials, it will etch It will also stop automatically, which greatly facilitates the process control. The tartaric acid/hydrogen peroxide system is composed of tartaric acid and water diluted at a volume ratio of 1:1 and then added with 5 vol% hydrogen peroxide; the volume ratio of hydrochloric acid/phosphoric acid is 1:4, and the hydrochloric acid used is chemically pure or analytically pure.

根据探测器的紫外增强响应光谱要求,探测器工艺中我们选用了对紫外光透明的低折射率材料作为增透膜材料,并根据增加短波响应的要求采用了较薄的抗反射增透膜,可达到良好的紫外增强效果。实际器件制作工艺步骤如下:首先生长出砷化镓基含磷材料的紫外增强光电探测器的外延结构,检测合格后采用光刻方法刻出台面图形,用选择腐蚀方法刻蚀出台面结构,经清洗后进行表面钝化并在钝化层上刻出进光窗口,再光刻出电极图形,采用蒸发和剥离方法制作出接触电极,经合金化后用选择腐蚀方法除去进光窗口上的GaAs上接触层,然后用蒸发方法制作抗反射增透膜并除去其不需要的部分,最后经衬底减薄抛光、划片、崩片等工艺后得到探测器管芯。探测器管芯经初步筛选后根据需要进行相应的封装,然后进行性能测试。According to the requirements of the enhanced ultraviolet response spectrum of the detector, in the detector process, we selected a low refractive index material transparent to ultraviolet light as the anti-reflection coating material, and adopted a thinner anti-reflection anti-reflection coating according to the requirement of increasing the short-wave response. Good UV enhancement effect can be achieved. The actual device manufacturing process steps are as follows: First, the epitaxial structure of the ultraviolet-enhanced photodetector of the gallium arsenide-based phosphorus-containing material is grown. After cleaning, the surface is passivated and the light entrance window is engraved on the passivation layer, and then the electrode pattern is photoetched, and the contact electrode is produced by evaporation and stripping. After alloying, the GaAs on the light entrance window is removed by selective etching. The upper contact layer, and then use the evaporation method to make anti-reflection and anti-reflection film and remove its unnecessary parts, and finally obtain the detector core after substrate thinning and polishing, scribing, chipping and other processes. After preliminary screening, the detector dies are packaged accordingly as required, and then performance tests are performed.

所述的增透膜材料的折射率范围为1.8-1.9,例如ZrO2或Al2O3中一种。The refractive index range of the anti-reflection coating material is 1.8-1.9, such as one of ZrO 2 or Al 2 O 3 .

所述的外延结构生长包括:The growth of the epitaxial structure comprises:

(1)首先在GaAs衬底上生长高掺杂Si的n型低阻GaAs下接触层;(1) First grow a highly doped Si n-type low-resistance GaAs lower contact layer on the GaAs substrate;

(2)在步骤(1)生长的下接触层上生长低掺杂Si或不掺杂Si的含磷化合物光吸收层;(2) growing a low-doped Si or non-doped Si-containing phosphorous compound light absorbing layer on the lower contact layer grown in step (1);

(3)在步骤(2)生长的吸收层上生长高掺杂Be的P型含磷化合物的光吸收层,然后在其上生长高掺杂的P型含磷的化合物窗口层;(3) growing a light absorbing layer of a P-type phosphorus-containing compound highly doped with Be on the absorption layer grown in step (2), and then growing a highly doped P-type phosphorus-containing compound window layer thereon;

(4)最后在步骤(3)生长的窗口层上生长高掺杂的P型低阻GaAs上接触层;(4) Finally, on the window layer grown in step (3), a highly doped P-type low-resistance GaAs upper contact layer is grown;

此种新型紫外增强光电探测器在火焰探测、光度测量、尾焰跟踪、生物及化学气体检测以及紫外线防护等方面都可发挥重要作用。例如:采用AlInP/GaInP/GaAs外延结构的探测器(如实施例1及附图4所示)的光谱响应与人眼的视觉敏感光谱响应(及标准C.I.E曲线)十分吻合,因此此探测器可直接应用于照度测量;再如:此探测器在蓝、绿光波长上有很好的响应并扩展到近紫外波段,因此也是合适的尾焰跟踪(如导弹双色制导)和火焰探测器件。This new type of UV-enhanced photodetector can play an important role in flame detection, photometry, tail flame tracking, biological and chemical gas detection, and ultraviolet protection. For example: the spectral response of the detector (as shown in embodiment 1 and accompanying drawing 4) that adopts AlInP/GaInP/GaAs epitaxial structure is very consistent with the visual sensitivity spectral response (and standard C.I.E curve) of human eyes, so this detector can It is directly applied to illuminance measurement; another example: this detector has a good response in blue and green light wavelengths and extends to the near ultraviolet band, so it is also suitable for tail flame tracking (such as missile two-color guidance) and flame detection devices.

附图说明Description of drawings

图1是本发明提供的基于砷化镓基含磷化合物半导体材料的紫外增强光电探测器的示意图。图中1:半绝缘砷化镓衬底,2:宽禁带含磷光吸收层,3:窗口层,4:PN结,5:钝化层,6:下接触层,7:下电极,8:上电极,9:增透膜,10:上接触层FIG. 1 is a schematic diagram of an ultraviolet-enhanced photodetector based on gallium arsenide-based phosphorus-containing compound semiconductor materials provided by the present invention. In the figure 1: semi-insulating gallium arsenide substrate, 2: wide band gap containing phosphorescent absorbing layer, 3: window layer, 4: PN junction, 5: passivation layer, 6: lower contact layer, 7: lower electrode, 8 : upper electrode, 9: AR coating, 10: upper contact layer

图2为按实施例1制作的AlInP/GaInP/GaAs紫外增强光电探测器的典型I-V特性Fig. 2 is the typical I-V characteristic of the AlInP/GaInP/GaAs ultraviolet enhanced photodetector made according to embodiment 1

图3为按实施例1制作的AlInP/GaInP/GaAs紫外增强光电探测器在零偏压附近的I-V特性Fig. 3 is the I-V characteristic of the AlInP/GaInP/GaAs ultraviolet enhanced photodetector made according to embodiment 1 near zero bias voltage

图4为按实施例1制作的AlInP/GaInP/GaAs紫外增强光电探测器的响应光谱(虚线为人眼视觉敏感标准C.I.E曲线)Fig. 4 is the response spectrum of the AlInP/GaInP/GaAs ultraviolet enhanced photodetector made by embodiment 1 (the dotted line is the C.I.E curve of the human eye visual sensitivity standard)

具体实施方式Detailed ways

下面通过附图的实施例进一步说明本发明的实质性的特点和显著的进步,但绝非限制本发明,即本发明绝非仅局限于实施例。The substantive features and remarkable progress of the present invention are further described below through the embodiments of the accompanying drawings, but the present invention is by no means limited, that is, the present invention is by no means limited to the embodiments.

实施例1:Example 1:

采用气态源分子束外延(GSMBE)方法生长Al0.52In0.48P/Ga0.51In0.49P/GaAs紫外增强光电探测器Al 0.52 In 0.48 P/Ga 0.51 In 0.49 P/GaAs UV-Enhanced Photodetectors Grown by Gas Source Molecular Beam Epitaxy (GSMBE)

一、制作实施步骤:1. Production and implementation steps:

1.采用气态源分子束外延(GSMBE)方法生长Al0.52In0.48P/Ga0.51In0.49P/GaAs紫外增强光电探测器材料。首先根据晶格匹配条件确定Ga0.51In0.49P和Al0.52In0.48P单层材料的生长工艺,在470℃的衬底温度和450Torr的P源压力及850℃In束源温度的条件下确定Ga和Al的束源温度使GaInP和AlInP单层材料与GaAs衬底的失配度控制在+5×10-4左右,生长速率控制在0.5-1μm/h。在此过程中同时确定Be掺杂温度使载流子浓度>1E18cm-31. Al 0.52 In 0.48 P/Ga 0.51 In 0.49 P/GaAs UV-enhanced photodetector materials were grown by gas source molecular beam epitaxy (GSMBE). Firstly, the growth process of Ga 0.51 In 0.49 P and Al 0.52 In 0.48 P single-layer materials is determined according to the lattice matching conditions, and the Ga The beam source temperature of Al and Al can control the mismatch between GaInP and AlInP single-layer materials and GaAs substrate at about +5×10 -4 , and control the growth rate at 0.5-1 μm/h. During this process, the Be doping temperature is determined at the same time so that the carrier concentration is greater than 1E18cm -3 .

2.在优化的生长条件下生长探测器的器件结构。首先生长厚度0.8-1.5μm的高掺Si(n>5×1017cm-3)n型低阻GaAs下接触层,在其上生长厚度为0.5-1μm的低掺Si(n<5×1017cm-3)或不掺杂n型Ga0.51In0.49P光吸收层,具体厚度可根据具体器件要求确定(希望抑制长波响应时可选用较薄的外延层,但量子效率会有所降低);再在其上生长厚度为30nm的高掺Be(p>5×1017cm-3)p型Ga0.51In0.49P光吸收层,然后在其上生长厚度为20-30nm的高掺Be(p>5×1017cm-3)p型Al0.52In0.48P窗口层,最后生长厚度为0.2-0.5μm的高掺Be(p>5×1017cm-3)p型低阻GaAs上接触层。2. Grow the device structure of the detector under optimized growth conditions. First grow a high-doped Si (n>5×10 17 cm -3 ) n-type low-resistance GaAs lower contact layer with a thickness of 0.8-1.5 μm, and grow a low-doped Si (n<5×10 17 cm -3 ) or undoped n-type Ga 0.51 In 0.49 P light absorbing layer, the specific thickness can be determined according to the specific device requirements (thinner epitaxial layer can be used when it is desired to suppress long-wave response, but the quantum efficiency will be reduced) and then grow a p-type Ga 0.51 In 0.49 P light absorbing layer with a thickness of 30nm on it, and then grow a highly doped Be ( p>5×10 17 cm -3 ) p-type Al 0.52 In 0.48 P window layer, and finally grow a high-doped Be (p>5×10 17 cm -3 ) p-type low-resistance GaAs upper contact with a thickness of 0.2-0.5 μm layer.

3.生长好的外延片经显微镜检、结构特性(X-ray测量晶格匹配等)和电学特性(电化学C-V测量载流子浓度等)检测合格后进行器件工艺制作。先采用光刻方法刻出台面图形,用选择腐蚀方法刻蚀出台面结构,经清洗后进行表面钝化并在钝化层上刻出进光窗口,再光刻出电极图形,采用蒸发和剥离方法制作出接触电极,经合金化后用选择腐蚀方法除去进光窗口上的GaAs上接触层,然后用蒸发方法制作抗反射增透膜并除去其不需要的部分,最后经衬底减薄抛光、划片、崩片等工艺后得到探测器管芯。3. After the grown epitaxial wafer is qualified by microscope inspection, structural characteristics (X-ray measurement of lattice matching, etc.) and electrical characteristics (electrochemical C-V measurement of carrier concentration, etc.), the device process is carried out. First use photolithography to carve out the mesa pattern, use selective etching to etch the mesa structure, passivate the surface after cleaning and carve the light entrance window on the passivation layer, and then photoetch the electrode pattern, use evaporation and stripping The method is to make the contact electrode, remove the GaAs upper contact layer on the light entrance window by selective etching after alloying, then make the anti-reflection and anti-reflection film by evaporation method and remove its unnecessary part, and finally polish it by thinning the substrate , scribing, chipping and other processes to obtain the detector core.

4.探测器管芯经初步筛选后根据需要进行相应的封装,制成探测器。4. The detector core is preliminarily screened and packaged accordingly as required to make a detector.

二、探测器的特性:Second, the characteristics of the detector:

图2为采用以上工艺制作的Al0.52In0.48P/Ga0.51In0.49P/GaAs紫外增强光电探测器的典型I-V特性,其击穿电压>5V,0.5V反偏压下的暗电流小于5pA,图3为其在零偏压附近的I-V特性,其零偏电阻R0高达8×104MΩ。图4为探测器的响应光谱,响应波长范围为250-650nm,峰值响应波长约580nm.与硅光电探测器相比,本实施例提供的探测器对红外光的响应已被完全抑制,光照下的输出电压也有大幅度提高。Figure 2 shows the typical IV characteristics of the Al 0.52 In 0.48 P/Ga 0.51 In 0.49 P/GaAs UV-enhanced photodetector fabricated by the above process, the breakdown voltage is >5V, and the dark current under 0.5V reverse bias is less than 5pA Figure 3 shows its IV characteristics near zero bias voltage, and its zero bias resistance R 0 is as high as 8×10 4 MΩ. Figure 4 is the response spectrum of the detector, the response wavelength range is 250-650nm, and the peak response wavelength is about 580nm. Compared with silicon photodetectors, the detector provided in this embodiment has been completely suppressed in response to infrared light. The output voltage is also greatly improved.

实施例2:Example 2:

采用GSMBE生长方法生长Al0.52In0.48P/Al0.28Ga0.23In0.49P/GaAs紫外增强光电探测器Growth of Al 0.52 In 0.48 P/Al 0.28 Ga 0.23 In 0.49 P/GaAs UV-enhanced photodetectors grown by GSMBE growth method

制作实施步骤:Production implementation steps:

1.采用气态源分子束外延(GSMBE)方法生长Al0.52In0.48P/Al0.28Ga0.23In0.49P/GaAs紫外增强光电探测器材料。首先根据晶格匹配条件确定Al0.28Ga0.23In0.49P和Al0.52In0.48P单层材料的生长工艺,在470℃的衬底温度和450Torr的P源压力及850℃ In束源温度的条件下确定In、Ga和Al的束源温度使AlGaInP和AlInP单层材料与GaAs衬底的失配度控制在+5×10-4左右,生长速率控制在0.5-1μm/h。在此过程中同时确定Be掺杂温度使载流子浓度>1E18cm-31. Al 0.52 In 0.48 P/Al 0.28 Ga 0.23 In 0.49 P/GaAs UV-enhanced photodetector materials were grown by gas source molecular beam epitaxy (GSMBE). Firstly, the growth process of Al 0.28 Ga 0.23 In 0.49 P and Al 0.52 In 0.48 P single-layer materials is determined according to the lattice matching conditions. Under the conditions of substrate temperature of 470°C, P source pressure of 450 Torr and In beam source temperature of 850°C Determine the beam source temperature of In, Ga and Al so that the mismatch between AlGaInP and AlInP single-layer materials and GaAs substrate is controlled at about +5×10 -4 , and the growth rate is controlled at 0.5-1 μm/h. During this process, the Be doping temperature is determined at the same time so that the carrier concentration is greater than 1E18cm -3 .

2.在优化的生长条件下生长探测器的器件结构。首先生长厚度0.8-1.5μm的高掺Si(n>5×1017cm-3)n型低阻GaAs下接触层,在其上生长厚度为0.5-1μm(根据具体器件要求)的低掺Si(n<5×1017cm-3)或不掺杂的n型Al0.28Ga0.23In0.49P光吸收层,再在其上生长厚度为30nm的高掺Be(p>5×1017cm-3)p型Al0.28Ga0.23In0.49P光吸收层,然后在其上生长厚度为20-30nm的高掺Be(p>5×1017cm-3)p型Al0.52In0.48P窗口层,最后生长厚度为0.2-0.5μm的高掺Be(p5×1017cm-3)p型低阻GaAs上接触层。2. Grow the device structure of the detector under optimized growth conditions. First grow a high-doped Si (n>5×10 17 cm -3 ) n-type low-resistance GaAs lower contact layer with a thickness of 0.8-1.5 μm, and grow low-doped Si with a thickness of 0.5-1 μm (according to specific device requirements) on it (n<5×10 17 cm -3 ) or undoped n-type Al 0.28 Ga 0.23 In 0.49 P light absorbing layer, and then grow highly doped Be (p>5×10 17 cm -3 ) with a thickness of 30nm on it 3 ) p-type Al 0.28 Ga 0.23 In 0.49 P light absorbing layer, and then grow a highly Be-doped (p>5×10 17 cm -3 ) p-type Al 0.52 In 0.48 P window layer with a thickness of 20-30 nm on it, Finally, a high-doped Be (p5×10 17 cm -3 ) p-type low-resistance GaAs upper contact layer is grown with a thickness of 0.2-0.5 μm.

3.生长好的外延片经显微镜检、结构特性(X-ray测量晶格匹配等)和电学特性(电化学C-V测量载流子浓度等)检测合格后进行器件工艺制作。先采用光刻方法刻出台面图形,用选择腐蚀方法刻蚀出台面结构,经清洗后进行表面钝化并在钝化层上刻出进光窗口,再光刻出电极图形,采用蒸发和剥离方法制作出接触电极,经合金化后用选择腐蚀方法除去进光窗口上的GaAs上接触层,然后用蒸发方法制作抗反射增透膜并除去其不需要的部分,最后经衬底减薄抛光、划片、崩片等工艺后得到探测器管芯。3. After the grown epitaxial wafer is qualified by microscope inspection, structural characteristics (X-ray measurement of lattice matching, etc.) and electrical characteristics (electrochemical C-V measurement of carrier concentration, etc.), the device process is carried out. First use photolithography to carve out the mesa pattern, use selective etching to etch the mesa structure, passivate the surface after cleaning and carve the light entrance window on the passivation layer, and then photoetch the electrode pattern, use evaporation and stripping The method is to make the contact electrode, remove the GaAs upper contact layer on the light entrance window by selective etching after alloying, then make the anti-reflection and anti-reflection film by evaporation method and remove its unnecessary part, and finally polish it by thinning the substrate , scribing, chipping and other processes to obtain the detector core.

4.探测器管芯经初步筛选后根据需要进行相应的封装,制成探测器。4. The detector core is preliminarily screened and packaged accordingly as required to make a detector.

经测定,采用以上工艺制作的Al0.52In0.48P/Al0.28Ga0.23In0.49P/GaAs紫外增强光电探测器的截止波长可比Al0.52In0.48P/Ga0.51In0.49P/GaAs紫外增强光电探测器进一步减小,探测器对红外光的响应可被完全抑制,对红光的响应也可部分抑制,紫外增强效果可进一步加强。It has been determined that the cut-off wavelength of the Al 0.52 In 0.48 P/Al 0.28 Ga 0.23 In 0.49 P/GaAs UV-enhanced photodetector produced by the above process is comparable to that of the Al 0.52 In 0.48 P/Ga 0.51 In 0.49 P/GaAs UV-enhanced photodetector If it is further reduced, the detector's response to infrared light can be completely suppressed, and the response to red light can also be partially suppressed, and the ultraviolet enhancement effect can be further strengthened.

Claims (9)

1, a kind of ultraviolet reinforced photo detector that adopts gallium arsenide base phosphorated material, it is characterized in that adopting the semi-insulating GaAs monocrystal material of doping as substrate of detector, adopt epitaxially grown broad stopband phosphorus-containing compound film as active light absorbing zone and Window layer thereon, and between absorption window and Window layer, constitute PN junction, and adopt single-side electrode to draw.
2, by the ultraviolet reinforced photo detector of the described employing gallium arsenide base phosphorated material of claim 1, it is characterized in that described broad stopband phosphorus-containing compound is the Ga of ternary system 0.51In 0.49P, Al 0.52In 0.48(the Al of P or quaternary system zGa 1-z) 0.51In 0.49P, 0<Z<0.55.
3, by the ultraviolet reinforced photo detector of the described employing gallium arsenide base phosphorated material of claim 2, it is characterized in that described Ga 0.51In 0.49P, Al 0.52In 0.48P is the direct band gap material, and the band gap material under the room temperature is 1.85eV; (Al zGa 1-z) 0.51In 0.49P is an indirect bandgap material, and band gap is 2.34eV.
4, by the ultraviolet reinforced photo detector of the described employing gallium arsenide base phosphorated material of claim 1, it is characterized in that as substrate of detector be highly doped N type conductive substrates, detector adopts the double-face electrode structure.
5, make the method for the ultraviolet reinforced photo detector of employing gallium arsenide base phosphorated material as claimed in claim 1, it is characterized in that concrete making step is:
(1) at first on the GaAs substrate growth highly doped Si n type low-resistance GaAs under contact layer;
(2) the phosphorus-containing compound light absorbing zone of the low-doped Si of growth or the Si that undopes on the following contact layer of step (1) growth;
(3) light absorbing zone of the P type phosphorus-containing compound of the highly doped Be of growth on the absorbed layer of step (2) growth, the compound Window layer that the P type of growing highly doped thereon then is phosphorous;
(4) at last on the Window layer of step (3) growth the highly doped P type low-resistance GaAs of growth go up contact layer;
(5) carrying out device technology at the good epitaxial wafer of step (1)~(4) growths after after testing makes, adopt photoetching method to carve the table top figure earlier, etch mesa structure with the selective etching method, after cleaning, carry out surface passivation and on passivation layer, carve light portal, make electrode pattern again by lithography, adopt evaporation and stripping means to produce contact electrode, GaAs through removing on the light portal with the selective etching method after the alloying goes up contact layer, make the antireflection anti-reflection film and remove its unwanted part with method of evaporating then, after the substrate thinning polishing, scribing, obtain probe dice after the technologies such as disintegrating tablet;
(6) probe dice encapsulates after Preliminary screening as required accordingly, makes detector.
6, press the manufacture method of the ultraviolet reinforced photo detector of the described employing gallium arsenide base phosphorated material of claim 5, it is characterized in that in epitaxial wafer growth step (1)~(4):
(1) contact layer thickness is 0.8-1.5 μ m under the n type of described highly doped Si, and doping content is greater than 5 * 10 17Cm -3
(2) described low-doped Si or plain n type phosphorus-containing compound, light absorption thickness is 0.5-1 μ m, low-doped Si concentration is less than 5 * 10 17Cm -3
(3) described on the light absorbing zone of the low-doped Si or the Si that undopes the regeneration P type phosphorus-containing compound thickness of mixing Be that grows tall be 30nm, the concentration of doping Be is greater than 5 * 10 17Cm -3
(4) described Window layer is the high p type phosphorus-containing compound of mixing Be, and growth thickness is 20-30nm, and the concentration of doping Be is greater than 5 * 10 17Cm -3
(5) described upward contact layer thickness is 0.2-0.5 μ m, and the concentration of doping Be is greater than 5 * 10 17Cm -3
7, press the manufacture method of the ultraviolet reinforced photo detector of claim 5 or 6 described employing gallium arsenide base phosphorated materials, it is characterized in that epitaxial growth is a kind of in employing molecular beam epitaxy or the gas phase epitaxy of metal organic compound method.
8, press the manufacture method of the ultraviolet reinforced photo detector of claim 5 or 6 described employing gallium arsenide base phosphorated materials, the material that it is characterized in that light absorbing zone is Ga 0.51In 0.49P or (Al zGa 1-z) 0.51In 0.49P, a kind of in 0<Z<0.55, window material is Al 0.52In 0.48P, the refractive index of anti-reflection film material is the ZrO of 1.8-1.9 2Or Al 2O 3In a kind of.
9, press the manufacture method of the ultraviolet reinforced photo detector of the described employing gallium arsenide base phosphorated material of claim 5, utilize tartaric acid/hydrogen peroxide corrosive liquid etching GaAs material when it is characterized in that selective etching, etching stops automatically when running into the phosphorus-containing compound material; Utilize hydrochloric acid/phosphoric acid system etching phosphorus-containing compound, etching stops automatically when running into not phosphorus-containing compound.
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