CN116913768A - Multiple pulse sub-melting excimer laser annealing method - Google Patents
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Abstract
Description
技术领域Technical field
本发明属于半导体技术领域,具体地,涉及一种多次脉冲亚熔化准分子激光退火方法。The invention belongs to the field of semiconductor technology, and specifically relates to a multi-pulse sub-melting excimer laser annealing method.
背景技术Background technique
随着半导体器件的快速发展,对其性能的要求越来高,因而对其加工工艺提出了更多特殊的要求。例如,由于半导体芯片特征尺寸的不断缩小,晶体管的源漏区需要更低的电阻和超浅结(ultra-shallow junction,USJ)才能减少短通道效应,即掺杂深度越来越浅,而掺杂浓度越来越高。通过降低注入离子能量形成浅结的方法一直受到本领域的重视,同时高活化USJ的制备已成为现代掺杂工艺的一个最大挑战,这要求极低的离子注入的能量以及超高的掺杂浓度。With the rapid development of semiconductor devices, the requirements for their performance are getting higher and higher, which puts forward more special requirements for their processing technology. For example, due to the continuous shrinkage of semiconductor chip feature sizes, the source and drain regions of transistors require lower resistance and ultra-shallow junctions (USJ) to reduce the short channel effect, that is, the doping depth becomes shallower and shallower, and the doping depth becomes shallower and shallower. The impurity concentration is getting higher and higher. The method of forming shallow junctions by reducing the implanted ion energy has always attracted attention in this field. At the same time, the preparation of highly activated USJ has become one of the biggest challenges in modern doping processes, which requires extremely low ion implantation energy and ultra-high doping concentration. .
在相关技术中,为了形成高活化的浅结轮廓,低能束流式离子注入技术和浸没式等离子体注入技术被广泛用于半导体晶元中以引入掺杂剂。在注入结束后使用闪光灯退火(flash lamp annealing,FLA)和尖峰快速热退火(spike-RTA)等方式来消除注入损伤并激活掺杂剂。然而,由于退火时间长且杂质激活程度有限,FLA和spike-RTA并不适合形成高活化水平的超浅结。In the related art, in order to form a highly activated shallow junction profile, low-energy beam ion implantation technology and immersion plasma implantation technology are widely used in semiconductor wafers to introduce dopants. After the implantation is completed, methods such as flash lamp annealing (FLA) and spike rapid thermal annealing (spike-RTA) are used to eliminate implant damage and activate dopants. However, due to the long annealing time and limited impurity activation, FLA and spike-RTA are not suitable for forming ultra-shallow junctions with high activation levels.
在半导体领域,硅基高效发光材料和器件的研究是热点之一,现有技术中曾提出一种兼容硅CMOS工艺的直接带隙硅基发光材料制备方法,利用离子注入技术向晶体锗中置入浓度超过1%的惰性原子来促使其晶格膨胀产生等效张应变,以此实现间接带隙向直接带隙的转换,从而实现高效发光。此外,通过向锗中置入特定浓度的锗或锡原子形成分裂的[110]间隙位等电子掺杂后也可实现直接带隙发光。然而,无论闭壳层的惰性气体原子掺杂还是等电子的锗原子和锡原子掺杂,在单晶锗中的平衡固溶度均远小于1%,在修复因掺杂引起的晶格损伤时会导致大量的掺杂原子从表面逃逸。In the field of semiconductors, research on silicon-based high-efficiency luminescent materials and devices is one of the hot spots. In the existing technology, a direct bandgap silicon-based luminescent material preparation method compatible with the silicon CMOS process has been proposed, using ion implantation technology to implant germanium in the crystal. Inert atoms with a concentration of more than 1% are introduced to cause the lattice expansion to produce equivalent tensile strain, thereby realizing the conversion of the indirect band gap to the direct band gap, thereby achieving efficient light emission. In addition, direct band gap luminescence can also be achieved by placing a specific concentration of germanium or tin atoms into germanium to form split [110] interstitial sites and other electron doping. However, regardless of whether the closed-shell layer is doped with inert gas atoms or isoelectronic germanium atoms and tin atoms, the equilibrium solid solubility in single crystal germanium is far less than 1%. It is difficult to repair the lattice damage caused by doping. This will cause a large number of dopant atoms to escape from the surface.
单脉冲准分子激光退火(Excimer Laser Annealing,ELA)技术可对受损的半导体材料进行重结晶并激活杂质。其纳秒级的退火周期可以大幅缩短退火时间并提高退火温度,因而具备更高的杂质激活效率,同时其有效退火深度可由激光能量密度精确控制。因此,单脉冲准分子激光退火技术在低电阻超浅结的制备方面具有巨大的应用潜力。Single-pulse excimer laser annealing (ELA) technology can recrystallize damaged semiconductor materials and activate impurities. Its nanosecond-level annealing cycle can significantly shorten the annealing time and increase the annealing temperature, so it has higher impurity activation efficiency. At the same time, its effective annealing depth can be precisely controlled by the laser energy density. Therefore, single-pulse excimer laser annealing technology has great application potential in the preparation of low-resistance ultra-shallow junctions.
然而,进一步研究发现,单辐照的单脉冲准分子激光退火处理通常需要较高的激光能量密度以激活掺杂剂。这使得材料基体表面处于熔化态,在快速冷却过程中通过液相外延结晶机制获得高质量再生层,其高温熔融-冷却结晶机理具有其固有缺陷:一方面,熔融的掺杂层在快速凝固结晶时会引起基体表面波动,从而导致再生的基体表面粗化或起伏不平,不利于器件制备。另一方面,掺杂剂在熔体中会重新分布且在快速冷却结晶时会部分损失,因而在使用单脉冲准分子激光退火技术进行退火处理时面临严重的掺杂原子损失问题。However, further research found that single-irradiation single-pulse excimer laser annealing usually requires higher laser energy density to activate the dopants. This puts the surface of the material matrix in a molten state, and a high-quality regeneration layer is obtained through the liquid phase epitaxial crystallization mechanism during the rapid cooling process. Its high-temperature melting-cooling crystallization mechanism has its inherent flaws: on the one hand, the molten doped layer solidifies and crystallizes rapidly. It will cause fluctuations in the surface of the substrate, resulting in roughening or unevenness of the surface of the regenerated substrate, which is not conducive to device preparation. On the other hand, dopants will be redistributed in the melt and partially lost during rapid cooling and crystallization, thus facing serious doping atom loss problems when using single-pulse excimer laser annealing technology for annealing.
因此,提出一种退火技术在低电阻高活化的超浅结及直接带隙硅基发光材料的制备方面具有深远意义。Therefore, proposing an annealing technology is of far-reaching significance in the preparation of ultra-shallow junctions with low resistance and high activation and direct band gap silicon-based luminescent materials.
发明内容Contents of the invention
有鉴于此,为解决相关技术中的以及其他方面的至少一种技术问题,本发明提出了一种多次脉冲亚熔化准分子激光退火方法,包括:对半导体晶体表面进行离子注入,在半导体晶体表面形成非晶掺杂区;向非晶掺杂区进行多次脉冲激光辐照退火,以使非晶掺杂区在亚熔化状态发生重结晶,激活非晶掺杂区的离子。In view of this, in order to solve at least one technical problem in the related art and other aspects, the present invention proposes a multi-pulse sub-melting excimer laser annealing method, which includes: ion implantation on the surface of the semiconductor crystal; An amorphous doped area is formed on the surface; multiple pulse laser irradiation and annealing are performed on the amorphous doped area, so that the amorphous doped area recrystallizes in a sub-melted state and activates ions in the amorphous doped area.
根据本发明的实施例,重结晶过程为由晶体区向非晶掺杂区以固相外延结晶的方式逐层进行重结晶。According to embodiments of the present invention, the recrystallization process is performed layer by layer in a solid-phase epitaxial crystallization manner from the crystalline region to the amorphous doped region.
根据本发明的实施例,脉冲激光辐照的能量密度为半导体晶体的熔化阈值的80%~95%。According to embodiments of the present invention, the energy density of pulsed laser irradiation is 80% to 95% of the melting threshold of the semiconductor crystal.
根据本发明的实施例,脉冲激光辐照的频率小于20Hz。According to an embodiment of the present invention, the frequency of pulsed laser irradiation is less than 20 Hz.
根据本发明的实施例,脉冲激光包括准分子纳秒脉冲激光、飞秒脉冲激光、毫秒脉冲激光中的一种。According to an embodiment of the present invention, the pulse laser includes one of an excimer nanosecond pulse laser, a femtosecond pulse laser, and a millisecond pulse laser.
根据本发明的实施例,在重结晶过程,逐渐提高脉冲激光辐照的能量密度,以补偿非晶掺杂区反射率及热吸收系数变化对重结晶速率的影响。According to embodiments of the present invention, during the recrystallization process, the energy density of pulsed laser irradiation is gradually increased to compensate for the impact of changes in reflectivity and heat absorption coefficient of the amorphous doped region on the recrystallization rate.
根据本发明的实施例,半导体晶体包括元素半导体、化合物半导体中的一种,优选为硅、锗、碳化硅、氮化镓中的一种。According to embodiments of the present invention, the semiconductor crystal includes one of elemental semiconductors and compound semiconductors, preferably one of silicon, germanium, silicon carbide, and gallium nitride.
根据本发明的实施例,半导体晶体结构类型包括块体结构或薄膜结构。According to embodiments of the present invention, the semiconductor crystal structure type includes a bulk structure or a thin film structure.
根据本发明的实施例,非晶掺杂区的掺杂类型包括n型掺杂、p型掺杂、等电子掺杂、惰性气体原子掺杂中的一种;优选地,惰性气体原子为氩原子。According to embodiments of the present invention, the doping type of the amorphous doped region includes one of n -type doping, p -type doping, isoelectronic doping, and inert gas atom doping; preferably, the inert gas atom is argon. atom.
根据本发明的实施例,离子注入包括束线式离子注入方法或等离子体浸没式离子注入方法。According to embodiments of the present invention, ion implantation includes a beam line ion implantation method or a plasma immersion ion implantation method.
根据本发明的实施例,非晶掺杂区的厚度小于300nm。According to embodiments of the present invention, the thickness of the amorphous doped region is less than 300 nm.
根据本发明的实施例,多次脉冲亚熔化准分子激光退火方法使得发生离子注入的非晶掺杂区在重结晶过程中始终保持固相状态,固相中极低的扩散速率使得离子注入分布基本不受热退火的影响,并且避免了表面烧蚀、蒸发效应以及熔体冷却再生引起杂质偏析效应,使得重结晶过程中的掺杂原子损失大幅降低。同时,由于非晶掺杂区处于亚熔化状态,不存液相外延结晶过程中因熔融波动造成的基体表面起伏及粗化现象,重结晶后可获得与初始注入表面类似的平坦的形貌特性。According to embodiments of the present invention, the multi-pulse sub-melting excimer laser annealing method allows the amorphous doped region where ions are implanted to always maintain a solid phase state during the recrystallization process, and the extremely low diffusion rate in the solid phase makes the ion implantation distribution It is basically not affected by thermal annealing, and avoids surface ablation, evaporation effects and impurity segregation effects caused by melt cooling and regeneration, greatly reducing the loss of doping atoms during the recrystallization process. At the same time, because the amorphous doped region is in a sub-melting state, there is no substrate surface undulation and roughening caused by melting fluctuations during the liquid phase epitaxial crystallization process. After recrystallization, a flat morphology similar to the initial injection surface can be obtained. .
附图说明Description of the drawings
图1是本发明实施例中多次脉冲亚熔化准分子激光退火方法流程图;Figure 1 is a flow chart of a multi-pulse sub-melting excimer laser annealing method in an embodiment of the present invention;
图2是本发明实施例中多次脉冲亚熔化准分子激光退火方法的重结晶原理图;Figure 2 is a schematic diagram of the recrystallization method of the multi-pulse sub-melting excimer laser annealing method in the embodiment of the present invention;
图3是本发明一实施例中氩离子注入后锗基体表面后多次脉冲亚熔化准分子激光退火方法流程图;其中,(a)是基体示意图、(b)是氩原子注入示意图、(c)是多次脉冲亚熔化准分子激光退火示意图;Figure 3 is a flow chart of a multi-pulse sub-melting excimer laser annealing method for the surface of a germanium substrate after argon ion implantation in an embodiment of the present invention; (a) is a schematic diagram of the substrate, (b) is a schematic diagram of argon atom implantation, (c) ) is a schematic diagram of multiple pulse sub-melting excimer laser annealing;
图4是本发明一实施例中氩离子注入后锗基体表面的高分辨透射电子显微形貌图;Figure 4 is a high-resolution transmission electron micrograph of the germanium substrate surface after argon ion implantation in one embodiment of the present invention;
图5是本发明一实施例中多脉冲亚熔化准分子脉冲激光退火后锗基体表面的高分辨透射电子显微形貌图;Figure 5 is a high-resolution transmission electron micrograph of the germanium substrate surface after multi-pulse sub-melting excimer pulse laser annealing in one embodiment of the present invention;
图6是本发明一实施例中基体锗材料在单脉冲液相外延结晶及多脉冲亚熔化固相外延结晶后的Ar原子掺杂分布对比曲线图。Figure 6 is a comparative curve chart of the Ar atom doping distribution of the base germanium material after single-pulse liquid-phase epitaxial crystallization and multi-pulse sub-melting solid-phase epitaxial crystallization in an embodiment of the present invention.
附图标记Reference signs
1、基体;1. Base body;
2、非晶掺杂区;2. Amorphous doped region;
3、非晶掺杂界面;3. Amorphous doping interface;
4、多次脉冲亚熔化准分子激光。4. Multiple pulse sub-melting excimer laser.
具体实施方式Detailed ways
为使本发明的目的、技术方案和优点更加清楚明白,以下结合具体实施例,并参照附图,对本发明作进一步的详细说明。In order to make the purpose, technical solutions and advantages of the present invention more clear, the present invention will be further described in detail below in conjunction with specific embodiments and with reference to the accompanying drawings.
在本发明中所公开的范围的端点和任何值都不限于该精确的范围或值,这些范围或值应当理解为包含接近这些范围或值的值。对于数值范围来说,各个范围的端点值之间、各个范围的端点值和单独的点值之间,以及单独的点值之间可以彼此组合而得到一个或多个新的数值范围,这些数值范围应被视为在本发明中具体公开。The endpoints of ranges and any values disclosed in this disclosure are not limited to the precise range or value, but these ranges or values are to be understood to include values approximating those ranges or values. For numerical ranges, the endpoint values of each range, the endpoint values of each range and individual point values, and the individual point values can be combined with each other to obtain one or more new numerical ranges. These values Ranges should be considered to be specifically disclosed in this disclosure.
在此使用的术语仅仅是为了描述具体实施例,而并非意在限制本发明。在此使用的术语“包括”、“包含”等表明了所述特征、步骤、操作和/或部件的存在,但是并不排除存在或添加一个或多个其他特征、步骤、操作或部件。The terminology used herein is for the purpose of describing specific embodiments only and is not intended to be limiting of the invention. The terms "comprising," "comprising," and the like, as used herein, indicate the presence of stated features, steps, operations, and/or components but do not exclude the presence or addition of one or more other features, steps, operations, or components.
在此使用的所有术语(包括技术和科学术语)具有本领域技术人员通常所理解的含义,除非另外定义。应注意,这里使用的术语应解释为具有与本说明书的上下文相一致的含义,而不应以理想化或过于刻板的方式来解释。All terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art, unless otherwise defined. It should be noted that the terms used here should be interpreted to have meanings consistent with the context of this specification and should not be interpreted in an idealized or overly rigid manner.
类似地,为了精简本发明并帮助理解各个公开方面中的一个或多个,在上面对本发明示例性实施例的描述中,本发明的各个特征有时被一起分到单个实施例、图或者对其描述中。参考术语“一个实施例”、“一些实施例”、“示例”、“具体示例”、或“一些示例”等的描述意指结合该实施例或示例描述的具体特征、结构、材料或者特点包含于本发明的至少一个实施例或示例中。本说明书中,对上述术语的示意性表述不一定指的是相同的实施例或示例。而且,描述的具体特征、结构、材料或者特点可以在任何的一个或者多个实施例或示例中以合适的方式结合。Similarly, in the above description of exemplary embodiments of the invention, in order to streamline the invention and assist in understanding one or more of the various disclosed aspects, various features of the invention are sometimes grouped together into a single embodiment, figure, or grouped together. In description. Reference to a description of the terms "one embodiment," "some embodiments," "an example," "a specific example," or "some examples" or the like means that a particular feature, structure, material, or characteristic described in connection with the embodiment or example includes In at least one embodiment or example of the invention. In this specification, schematic expressions of the above terms do not necessarily refer to the same embodiment or example. Furthermore, the specific features, structures, materials or characteristics described may be combined in any suitable manner in any one or more embodiments or examples.
在传统的激光退火工艺中,造成掺杂原子损失的主要因素有三个,包括高能激光辐照时的表面烧蚀效应、基体熔融时的表面蒸发效应以及熔体冷却再生时的杂质偏析效应。在这些因素的共同作用下,单脉冲准分子激光退火工艺处理使得退火重结晶后滞留在半导体基体内并被有效激活的掺杂原子大幅下降。In the traditional laser annealing process, there are three main factors causing the loss of dopant atoms, including the surface ablation effect during high-energy laser irradiation, the surface evaporation effect during matrix melting, and the impurity segregation effect during melt cooling and regeneration. Under the combined effect of these factors, the single-pulse excimer laser annealing process significantly reduces the number of doping atoms that remain in the semiconductor matrix and are effectively activated after annealing and recrystallization.
当半导体基体材料受到高于其熔化阈值的纳秒脉冲激光能量辐照后表面会发生熔融现象,融化前沿快速(~10m/s)向半导体基体材料内部穿透,直至辐照结束。随后,表面熔融层通过向半导体基体释放热量而凝固结晶,熔化前沿又快速回扫至表面,整个过程将在数十纳秒时间内完成,被称为非平衡液相外延结晶。在整个熔融-结晶过程中因激光辐照造成的表面烧蚀效应、高温熔体产生的表面蒸发效应以及熔体冷却再生引起的杂质偏析效应均会造成掺杂原子损失。When the semiconductor base material is irradiated with nanosecond pulse laser energy higher than its melting threshold, the surface will melt. The melting front rapidly (~10m/s) penetrates into the semiconductor base material until the irradiation ends. Subsequently, the surface molten layer solidifies and crystallizes by releasing heat to the semiconductor matrix, and the melting front quickly sweeps back to the surface. The entire process will be completed in tens of nanoseconds, which is called non-equilibrium liquid phase epitaxial crystallization. During the entire melting-crystallization process, the surface ablation effect caused by laser irradiation, the surface evaporation effect caused by high-temperature melt, and the impurity segregation effect caused by cooling and regeneration of the melt will all cause the loss of doping atoms.
为了解决该问题,本领域技术人员曾提出在单脉冲准分子激光退火(ExcimerLaser Annealing,ELA)技术处理前向基体表面沉积一层特定厚度的介质保护层。然而,后续研究发现,这种保护层在高能量的ELA处理时,会作为杂质污染源向基体引入不期望的杂质,该杂质通过与已有的n型或p型杂质相结合而使后者大量失活。因此表面沉积介质层并不是一种理想的解决方案。由于尚未找到合适的退火方案,传统单脉冲准分子激光退火在低电阻高活化的USJ及直接带隙硅基发光材料的制备方面将难以发挥其优势作用,致使其在未来前沿微电子及光电子技术领域的应用均受到很大限制。In order to solve this problem, those skilled in the art have proposed depositing a dielectric protective layer of a specific thickness on the surface of the substrate before single-pulse excimer laser annealing (ELA) technology. However, follow-up studies have found that this protective layer can act as a source of impurity contamination to introduce undesirable impurities into the matrix during high-energy ELA treatment. The impurities combine with existing n -type or p -type impurities to cause a large amount of the latter. Deactivated. Therefore surface depositing a dielectric layer is not an ideal solution. Since a suitable annealing scheme has not yet been found, traditional single-pulse excimer laser annealing will not be able to play its advantageous role in the preparation of low-resistance and high-activation USJs and direct bandgap silicon-based luminescent materials, resulting in its use in cutting-edge microelectronics and optoelectronics technologies in the future. Applications in various fields are greatly restricted.
在本发明中,通过略低于非晶掺杂区熔化阈值的脉冲激光能量对其进行连续多次辐照,保证非晶掺杂区在重结晶过程中始终处于固相,以固相外延结晶的方式实现重结晶生长。由于固相状态下掺杂原子具有极低的扩散速率,使得离子注入分布基本不受热退火的影响,因而由辐照造成的表面烧蚀效应、熔体表面蒸发效应以及冷却再生时引起的杂质偏析效应均可得到有效抑制。In the present invention, the amorphous doped region is continuously irradiated multiple times with pulsed laser energy slightly lower than the melting threshold to ensure that the amorphous doped region is always in the solid phase during the recrystallization process and is crystallized by solid phase epitaxy. way to achieve recrystallization growth. Due to the extremely low diffusion rate of dopant atoms in the solid state, the ion implantation distribution is basically not affected by thermal annealing. Therefore, the surface ablation effect caused by irradiation, the evaporation effect on the melt surface, and the segregation of impurities caused by cooling and regeneration The effects can be effectively suppressed.
图1是本发明实施例中多次脉冲亚熔化准分子激光退火方法流程图。Figure 1 is a flow chart of a multi-pulse sub-melting excimer laser annealing method in an embodiment of the present invention.
本公开提出了一种多次脉冲亚熔化准分子激光退火方法,如图1所示,包括以下步骤S1、步骤S2。This disclosure proposes a multi-pulse sub-melting excimer laser annealing method, as shown in Figure 1, including the following steps S1 and S2.
步骤S1:对半导体晶体表面进行离子注入,在半导体晶体表面形成非晶掺杂区。Step S1: Perform ion implantation on the surface of the semiconductor crystal to form an amorphous doped region on the surface of the semiconductor crystal.
步骤S2:向非晶掺杂区进行多次脉冲激光辐照退火,以使非晶掺杂区在亚熔化状态发生重结晶,激活非晶掺杂区的离子。Step S2: Perform multiple pulse laser irradiation and annealing on the amorphous doped region, so that the amorphous doped region recrystallizes in a sub-melted state and activates ions in the amorphous doped region.
根据本发明的实施例,多次脉冲亚熔化准分子激光退火方法使得发生离子注入的非晶掺杂区在重结晶过程中始终保持固相状态,这种以固相形式的极低的扩散速率使得离子注入分布基本不受热退火的影响,并且避免了表面烧蚀、蒸发效应以及熔体冷却再生引起杂质偏析效应,使得重结晶过程中的掺杂原子损失现象大幅降低。同时,由于非晶掺杂区处于亚熔化状态,不存液相外延结晶过程中因熔融波动造成的基体表面起伏及粗化现象,重结晶后可获得与初始注入表面类似的平坦的形貌特性。According to embodiments of the present invention, the multi-pulse sub-melting excimer laser annealing method allows the amorphous doped region where ions are implanted to always maintain a solid phase state during the recrystallization process. This extremely low diffusion rate in the solid phase form The ion implantation distribution is basically not affected by thermal annealing, and the impurity segregation effect caused by surface ablation, evaporation effects and melt cooling regeneration is avoided, greatly reducing the loss of doping atoms during the recrystallization process. At the same time, because the amorphous doped region is in a sub-melting state, there is no substrate surface undulation and roughening caused by melting fluctuations during the liquid phase epitaxial crystallization process. After recrystallization, a flat morphology similar to the initial injection surface can be obtained. .
图2是本发明实施例中多次脉冲亚熔化准分子激光退火方法的重结晶原理图。Figure 2 is a schematic diagram of the recrystallization method of the multi-pulse sub-melting excimer laser annealing method in the embodiment of the present invention.
根据本发明的实施例,如图2所示,随着非晶掺杂区2发生重结晶,非晶掺杂界面3发生移动。根据Arrhenius理论模型,在每一脉冲下,非晶掺杂界面3处原子仅能迁移数个原子层的距离,这意味每一脉冲能够触发的结晶深度约为数个原子层。因此,为了使整个掺杂层彻底完成重结晶,在亚熔化结晶模式下需要对基体进行多脉冲连续辐照。According to an embodiment of the present invention, as shown in FIG. 2 , as the amorphous doped region 2 recrystallizes, the amorphous doped interface 3 moves. According to the Arrhenius theoretical model, atoms at the three amorphous doping interfaces can only migrate a few atomic layers under each pulse, which means that the crystallization depth that each pulse can trigger is approximately several atomic layers. Therefore, in order to completely complete the recrystallization of the entire doped layer, the substrate needs to be irradiated with multiple pulses continuously in the sub-melting crystallization mode.
根据本发明的实施例,通过改变脉冲次数可以调控重结晶厚度。According to embodiments of the present invention, the recrystallization thickness can be controlled by changing the number of pulses.
根据本发明的实施例,重结晶过程为由晶体区向非晶掺杂区2以固相外延结晶的方式逐层进行重结晶。According to an embodiment of the present invention, the recrystallization process is performed layer by layer in a solid-phase epitaxial crystallization manner from the crystalline region to the amorphous doped region 2 .
根据本发明的实施例,在多次脉冲亚熔化准分子激光退火的作用下非晶掺杂区的重结晶方向由晶体区向非晶掺杂区2移动,即非晶掺杂界面3由晶体区向非晶掺杂区2发生移动。重结晶厚度由脉冲数量精确控制,以实现埋层式的结晶效果,从而可满足特定领域的结晶需要。According to the embodiment of the present invention, under the action of multiple pulse sub-melting excimer laser annealing, the recrystallization direction of the amorphous doped region moves from the crystal region to the amorphous doped region 2, that is, the amorphous doped interface 3 changes from the crystalline region to the amorphous doped region 2. The region moves toward the amorphous doped region 2. The recrystallization thickness is precisely controlled by the number of pulses to achieve a buried-layer crystallization effect, which can meet the crystallization needs of specific fields.
根据本发明的实施例,以低于非晶掺杂区熔化阈值的脉冲激光能量对其辐照时,其表面迅速升温至亚熔化状态,在每一脉冲结束后非晶掺杂区通过向底部基体释放热量冷却,因而重结晶方向自下而上(即由晶体区向非晶掺杂区移动)。According to embodiments of the present invention, when the amorphous doped region is irradiated with pulse laser energy lower than the melting threshold, its surface rapidly heats up to a sub-melting state. After each pulse, the amorphous doped region passes toward the bottom. The matrix releases heat and cools, so the recrystallization direction is from bottom to top (that is, moving from the crystalline region to the amorphous doped region).
根据本发明的实施例,脉冲激光辐照的能量密度为半导体晶体的熔化阈值的80%~95%,例如,可选为80%、83%、85%、90%、93%等,优选为90%。According to embodiments of the present invention, the energy density of pulsed laser irradiation is 80% to 95% of the melting threshold of the semiconductor crystal, for example, it can be 80%, 83%, 85%, 90%, 93%, etc., preferably 90%.
根据本发明的实施例,脉冲激光能量密度应略低于非晶掺杂区的熔化阈值,使得非晶掺杂区在辐照作用下始终处于亚熔化态。而非晶掺杂区非晶化越彻底,其缺陷含量越高,对应的热吸收系数越强,所需的激光能量密度将越低。此外,非晶掺杂区越深,对激光的热穿透要求越高,所需的激光能量密度就越高。因此,对于特定的基体材料,优化的激光能量密度取决于注入层深度及缺陷含量。According to embodiments of the present invention, the pulse laser energy density should be slightly lower than the melting threshold of the amorphous doped region, so that the amorphous doped region is always in a sub-melted state under irradiation. The more complete the amorphization of the amorphous doped region, the higher the defect content, the stronger the corresponding heat absorption coefficient, and the lower the required laser energy density will be. In addition, the deeper the amorphous doped region, the higher the thermal penetration requirements of the laser, and the higher the required laser energy density. Therefore, for a specific matrix material, the optimized laser energy density depends on the implantation layer depth and defect content.
根据本发明的实施例,脉冲激光辐照的频率小于20Hz,例如可选为5Hz、8Hz、10Hz、13Hz、16Hz、18Hz等。According to embodiments of the present invention, the frequency of pulsed laser irradiation is less than 20 Hz, for example, it can be selected as 5 Hz, 8 Hz, 10 Hz, 13 Hz, 16 Hz, 18 Hz, etc.
根据本发明的实施例,在多次脉冲亚熔化准分子激光退火过程中,每一脉冲对基体的作用应是独立的,即每次脉冲之间互不影响。然而,由于基体的热扩散效率有限,多脉冲辐照的热量累积效应可能会使基体发生表面熔化现象,因而脉冲频率不应太高。另一方面,为了缩短退火时间,以适用产业应用需要,激光辐照频率也不能太低。在综合考虑表面热效应及退火时间成本后,本发明中设定的入射频率一般应小于20Hz,具体数值取决于基体材料类型、注入损伤程度及入射激光参数等因素。According to embodiments of the present invention, during the multi-pulse sub-melting excimer laser annealing process, the effect of each pulse on the substrate should be independent, that is, each pulse should not affect each other. However, due to the limited thermal diffusion efficiency of the substrate, the heat accumulation effect of multi-pulse irradiation may cause surface melting of the substrate, so the pulse frequency should not be too high. On the other hand, in order to shorten the annealing time and meet the needs of industrial applications, the laser irradiation frequency cannot be too low. After comprehensively considering the surface thermal effect and annealing time cost, the incident frequency set in the present invention should generally be less than 20 Hz. The specific value depends on factors such as the type of base material, the degree of injection damage, and the incident laser parameters.
根据本发明的实施例,多次脉冲亚熔化准分子激光退火的脉冲数量应能够使非晶掺杂区完全结晶。According to embodiments of the present invention, the number of pulses of the multi-pulse sub-melting excimer laser annealing should be able to completely crystallize the amorphous doped region.
根据本发明的实施例,脉冲激光包括准分子纳秒脉冲激光、飞秒脉冲激光、毫秒脉冲激光中的一种。According to an embodiment of the present invention, the pulse laser includes one of an excimer nanosecond pulse laser, a femtosecond pulse laser, and a millisecond pulse laser.
根据本发明的实施例,本发明提出的多次脉冲亚熔化准分子激光退火方法本质上属于固相外延结晶,但纳秒脉冲引起的超快加热及冷却速率使其具备非平衡掺杂特性。According to embodiments of the present invention, the multi-pulse sub-melting excimer laser annealing method proposed by the present invention essentially belongs to solid-phase epitaxial crystallization, but the ultra-fast heating and cooling rates caused by nanosecond pulses make it possess non-equilibrium doping characteristics.
根据本发明的实施例,在重结晶过程,逐渐提高脉冲激光辐照的能量密度,以补偿非晶掺杂区反射率及热吸收系数变化对重结晶速率的影响。According to embodiments of the present invention, during the recrystallization process, the energy density of pulsed laser irradiation is gradually increased to compensate for the impact of changes in reflectivity and heat absorption coefficient of the amorphous doped region on the recrystallization rate.
根据本发明的实施例,随着重结晶过程的不断进行,非晶掺杂区残留深度将不断变薄,基体表面对入射激光的反射率及其热吸收系数也将不断变化,在激光辐照能量不变的情况下这种变化将使结晶速率略有降低。因此,为了获得均匀的重结晶速率,以利于精确控制重结晶厚度,在退火过程中可逐渐提高激光辐照能量密度,以此补偿反射率及热吸收系数变化对重结晶速率造成的影响。According to embodiments of the present invention, as the recrystallization process continues, the residual depth of the amorphous doped region will continue to become thinner, and the reflectivity of the substrate surface to the incident laser and its heat absorption coefficient will also continue to change. When the laser irradiation energy This change will slightly reduce the crystallization rate. Therefore, in order to obtain a uniform recrystallization rate and facilitate precise control of the recrystallization thickness, the laser irradiation energy density can be gradually increased during the annealing process to compensate for the impact of changes in reflectivity and heat absorption coefficient on the recrystallization rate.
根据本发明的实施例,半导体晶体包括元素半导体、化合物半导体中的一种,优选为硅、锗、碳化硅、氮化镓中的一种。According to embodiments of the present invention, the semiconductor crystal includes one of elemental semiconductors and compound semiconductors, preferably one of silicon, germanium, silicon carbide, and gallium nitride.
根据本发明的实施例,半导体晶体结构类型包括块体结构或薄膜结构,其中,薄膜结构包括但不限于SOI(Silicon-On-Insulator)或GOI(Germanium-On-Insulator)。According to embodiments of the present invention, semiconductor crystal structure types include bulk structures or thin film structures, where the thin film structures include but are not limited to SOI (Silicon-On-Insulator) or GOI (Germanium-On-Insulator).
根据本发明的实施例,非晶掺杂区的掺杂类型包括n型掺杂、p型掺杂、等电子掺杂、惰性气体原子掺杂中的一种;优选地,在应用于硅基发光器件时,惰性气体原子可选为氩原子。According to embodiments of the present invention, the doping type of the amorphous doping region includes one of n-type doping, p-type doping, isoelectronic doping, and inert gas atomic doping; preferably, when applied to silicon-based When using a light-emitting device, the inert gas atoms may be argon atoms.
根据本发明的实施例,为了避免惰性原子注入在基体中形成气泡结构而阻碍后续退火结晶,惰性原子注入剂量一般需小于5×1016/cm2。According to embodiments of the present invention, in order to prevent inert atom implantation from forming a bubble structure in the matrix and hindering subsequent annealing and crystallization, the inert atom implantation dose generally needs to be less than 5×10 16 /cm 2 .
根据本发明的实施例,离子注入包括束线式离子注入方法或等离子体浸没式离子注入方法。According to embodiments of the present invention, ion implantation includes a beam line ion implantation method or a plasma immersion ion implantation method.
根据本发明的实施例,非晶掺杂区的厚度小于300nm。According to embodiments of the present invention, the thickness of the amorphous doped region is less than 300 nm.
根据本发明的实施例,在产业线中为了快速判断多次脉冲亚熔化准分子激光退火后非晶掺杂区是否获得完全重结晶,可直接对样品进行在线式的非破坏性的拉曼(Raman)、X射线衍射谱(XRD)或光致光谱(PL)测试分析,并将其与同等测试条件下预先采集的高质量的单晶基体结果作对比,利用对应的特征峰半高宽或强度的变化来判断是否实现高质量的外延结晶。According to embodiments of the present invention, in order to quickly determine whether the amorphous doped region has been completely recrystallized after multiple-pulse sub-melting excimer laser annealing in the industrial line, online non-destructive Raman ( (Raman), The change in intensity is used to determine whether high-quality epitaxial crystallization is achieved.
需要说明的是,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的其他实施例,都属于本发明保护的范围。It should be noted that the described embodiments are only some of the embodiments of the present invention, rather than all of the embodiments. Based on the embodiments of the present invention, other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the scope of protection of the present invention.
实施例:Example:
在本实施例中,示意性举例说明惰性原子Ar掺杂的非晶基体锗材料的多次脉冲亚熔化准分子激光退火方法。In this embodiment, a multi-pulse sub-melting excimer laser annealing method of an amorphous matrix germanium material doped with inert atoms Ar is schematically illustrated.
图3是本发明一实施例中氩离子注入后锗基体表面后多次脉冲亚熔化准分子激光退火方法流程图。Figure 3 is a flow chart of a method for multiple pulse sub-melting excimer laser annealing of the germanium substrate surface after argon ion implantation in one embodiment of the present invention.
步骤S101:准备半导体块状锗作为基体1,如图3中的(a)所示。其中,基体1大小为2英寸,电阻为0.01-0.05Ω·cm,晶相为<110>,完全非晶化的锗的熔化阈值约为350mJ/cm2。Step S101: Prepare semiconductor bulk germanium as the substrate 1, as shown in (a) in Figure 3. Among them, the size of the substrate 1 is 2 inches, the resistance is 0.01-0.05Ω·cm, the crystal phase is <110>, and the melting threshold of completely amorphous germanium is about 350mJ/cm 2 .
步骤S102:在基体1的一侧进行惰性原子Ar注入,形成一层特定深度的Ar原子非晶掺杂区2,如图3中的(b)所示。其中,采用浸没式等离子体离子注入技术向基体1注入Ar原子,注入能量为5kV,注入剂量为1×1016/cm2,注入时腔体中Ar气的工作气压为10-3Pa,放电功率为500W,用于放电的矩形电压脉宽为10μs,脉冲频率为1kHz。Step S102: Carry out inert atomic Ar implantation on one side of the substrate 1 to form a layer of Ar atom amorphous doping region 2 with a specific depth, as shown in (b) in Figure 3 . Among them, immersion plasma ion implantation technology is used to inject Ar atoms into the substrate 1, the injection energy is 5kV, the injection dose is 1×10 16 /cm 2 , the working pressure of the Ar gas in the cavity during the injection is 10 -3 Pa, and the discharge The power is 500W, the rectangular voltage pulse width used for discharge is 10μs, and the pulse frequency is 1kHz.
图4是本发明一实施例中氩离子注入后锗基体表面的高分辨透射电子显微形貌图。Figure 4 is a high-resolution transmission electron micrograph of the surface of a germanium substrate after argon ion implantation in an embodiment of the present invention.
如图4所示,基体1表面约15nm的深度已完全非晶化,与其接触的下方晶格仍排布良好,两者之间具有清晰的过渡界面。As shown in Figure 4, the depth of about 15 nm on the surface of substrate 1 has been completely amorphous, and the underlying lattice in contact with it is still well arranged, with a clear transition interface between the two.
步骤S103:利用准分子纳秒脉冲激光对非晶掺杂区2进行多脉冲亚熔化辐照,非晶掺杂界面3自下而上移动,使其完全重结晶,如图3中的(c)所示。其中,采用XeCl准分子纳秒脉冲激光退火系统配备有光束匀化器,光束截面大小为5mm×5mm,且能量分布均匀。XeCl准分子纳秒脉冲激光波长为308nm,脉冲周期为28ns,所采用的激光能量密度为300mJ/cm2,脉冲频率为8Hz,脉冲数量为500。Step S103: Use an excimer nanosecond pulse laser to perform multi-pulse sub-melting irradiation on the amorphous doped region 2. The amorphous doped interface 3 moves from bottom to top to completely recrystallize it, as shown in (c in Figure 3 ) shown. Among them, the XeCl excimer nanosecond pulse laser annealing system is equipped with a beam homogenizer, the beam cross-section size is 5mm×5mm, and the energy distribution is uniform. The wavelength of the XeCl excimer nanosecond pulse laser is 308nm, the pulse period is 28ns, the laser energy density used is 300mJ/cm 2 , the pulse frequency is 8Hz, and the number of pulses is 500.
图5是本发明一实施例中多脉冲亚熔化准分子脉冲激光退火后锗基体表面的高分辨透射电子显微形貌图。Figure 5 is a high-resolution transmission electron micrograph of the germanium substrate surface after multi-pulse sub-melting excimer pulse laser annealing in one embodiment of the present invention.
如图5所示,多脉冲亚熔化激光辐照处理后,基体1的锗表面非晶掺杂区完全消失,锗晶格排布有效恢复,无残留的晶格缺陷,这意味着非晶掺杂区在亚熔化多脉冲激光退火作用下实现了高质量的外延结晶。As shown in Figure 5, after multi-pulse sub-melting laser irradiation treatment, the amorphous doped area on the germanium surface of substrate 1 completely disappeared, and the germanium lattice arrangement was effectively restored without residual lattice defects, which means that the amorphous doped area The impurity region achieves high-quality epitaxial crystallization under the action of sub-melting multi-pulse laser annealing.
为确认本实施例中多次脉冲亚熔化准分子激光退火方法使用前后基体中的Ar原子掺杂含量分布,采用二次离子质谱仪(SIMS)对其进行了掺杂元素分析。In order to confirm the Ar atom doping content distribution in the matrix before and after using the multiple pulse sub-melting excimer laser annealing method in this example, a secondary ion mass spectrometer (SIMS) was used to analyze the doping elements.
作为对比,采用单脉冲高能量的准分子纳秒脉冲激光退火对离子注入样品进行了液相外延结晶,激光能量密度为800mJ/cm2。在该脉冲激光辐照条件下,非晶掺杂区完全熔化,辐照结束后,熔融层以单晶基体为籽晶实现液相外延再生。对液相外延结晶后的Ar原子掺杂分布同样采用SIMS技术进行了分析,结果如图6所示。For comparison, single-pulse high-energy excimer nanosecond pulse laser annealing was used to perform liquid-phase epitaxial crystallization of ion-implanted samples. The laser energy density was 800mJ/cm 2 . Under this pulse laser irradiation condition, the amorphous doped region is completely melted. After the irradiation is completed, the molten layer uses the single crystal matrix as the seed crystal to achieve liquid phase epitaxial regeneration. The Ar atom doping distribution after liquid phase epitaxial crystallization was also analyzed using SIMS technology, and the results are shown in Figure 6.
图6是本发明一实施例中基体锗材料在单脉冲液相外延结晶及多脉冲亚熔化固相外延结晶后的Ar原子掺杂分布对比曲线图。Figure 6 is a comparative curve chart of the Ar atom doping distribution of the base germanium material after single-pulse liquid-phase epitaxial crystallization and multi-pulse sub-melting solid-phase epitaxial crystallization in an embodiment of the present invention.
如图6所示,在高能量单脉冲的液相外延结晶后基体中的Ar原子含量大幅下降,特别是靠近掺杂表面区域。然而,对于多脉冲亚熔化模式诱导的固相外延结晶,掺杂损失现象得到了大幅遏制,尤其是在表面高浓度非晶掺杂区,Ar含量损失程度更低。As shown in Figure 6, the Ar atom content in the matrix dropped significantly after high-energy single-pulse liquid-phase epitaxial crystallization, especially in the region close to the doped surface. However, for solid-phase epitaxial crystallization induced by multi-pulse sub-melting mode, the doping loss phenomenon is greatly suppressed, especially in the surface high-concentration amorphous doped region, where the Ar content loss is even lower.
如前所述,这与惰性原子在固相基体中的低扩散速率及超高的结晶速率有关,即在多脉冲超快固相外延结晶过程中,非晶层中大量的Ar原子没有足够时间从基体逃逸便被自下而上移动的结晶界面所捕获。由于相比惰性气体原子,常规的n型、p型或等电子掺杂原子能够与基体稳定成键,在重结晶过程中能够被再生基体俘获而进入晶格替代位。As mentioned before, this is related to the low diffusion rate of inert atoms in the solid phase matrix and the ultra-high crystallization rate. That is, in the multi-pulse ultrafast solid-phase epitaxial crystallization process, a large number of Ar atoms in the amorphous layer do not have enough time. Escape from the matrix is captured by the crystallographic interface moving from bottom to top. Compared with inert gas atoms, conventional n -type , p -type or isoelectronic doping atoms can stably form bonds with the matrix, and can be captured by the regenerated matrix during the recrystallization process and enter the lattice substitution site.
因而对于该类型掺杂原子采用多脉冲亚熔化模式结晶时可进一步降低杂质损失,从而有利于实现超高固溶度掺杂。Therefore, the multi-pulse sub-melting mode crystallization for this type of doped atoms can further reduce the loss of impurities, which is beneficial to achieving ultra-high solid solubility doping.
在本发明中,离子注入技术及多脉冲亚熔化激光退火技术均可兼容CMOS工艺,可大规模用于现有半导体技术产业,因此这种新型退火技术将成为未来制备低电阻USJ及新型直接带隙发光硅基材料的有利方案。In the present invention, both the ion implantation technology and the multi-pulse sub-melting laser annealing technology are compatible with the CMOS process and can be used on a large scale in the existing semiconductor technology industry. Therefore, this new annealing technology will become the future preparation method for low-resistance USJ and new direct tape. A favorable solution for gap-emitting silicon-based materials.
以上所述的具体实施例,对本发明的目的、技术方案和有益效果进行了进一步详细说明,应理解的是,以上所述仅为本发明的具体实施例而已,并不用于限制本发明,凡在本发明的精神和原则之内,所做的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The specific embodiments described above further describe the purpose, technical solutions and beneficial effects of the present invention in detail. It should be understood that the above are only specific embodiments of the present invention and are not intended to limit the present invention. Within the spirit and principles of the present invention, any modifications, equivalent substitutions, improvements, etc. shall be included in the protection scope of the present invention.
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