CN100565912C - High K Dielectric Film - Google Patents
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- CN100565912C CN100565912C CNB2004800334990A CN200480033499A CN100565912C CN 100565912 C CN100565912 C CN 100565912C CN B2004800334990 A CNB2004800334990 A CN B2004800334990A CN 200480033499 A CN200480033499 A CN 200480033499A CN 100565912 C CN100565912 C CN 100565912C
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Abstract
Description
技术领域 technical field
本发明涉及用于制造集成电路的装置和方法,更具体而言,涉及用于制造集成电路的高K电介质。The present invention relates to apparatus and methods for fabricating integrated circuits, and more particularly, to high-k dielectrics for fabricating integrated circuits.
背景技术 Background technique
CMOS器件包括n沟道和p沟道场效应晶体管(FET),并且形成集成电路的衬底。这些晶体管是基于金属氧化物的半导体器件,其包括源极区和漏极区以及其间的绝缘栅。随着集成电路的密度以及性能的增加,晶体管的尺寸必须减小。结果,绝缘栅介电层的厚度必须制造得更小。至于栅极电介质,该介电层的一个理想特性是它耦合上面的栅电极到下面的沟道,以使得该沟道可以响应施加到栅极的激励。在这个意义上,该电介质具有高介电常数是理想的,高介电常数就是人们熟知的高K。到目前为止,二氧化硅已经成为在制造集成电路时最常用和有效的栅极绝缘物。这具有非常高的集成度,特别是,能够在制造时具有非常低的缺陷密度。结果是,二氧化硅非常有效地运行,使得这些装置具有低的漏电流。不幸的是,随着栅极电介质的厚度减小,漏电流大大增加。例如,厚度小于20的SiO2导致不可接受的漏电流以及降低的装置性能。因此,需要在CMOS器件中替换SiO2。通过使较厚的高K层具有降低的等效(SiO2)氧化物厚度,可以减小漏电流。CMOS devices include n-channel and p-channel field effect transistors (FETs) and form the substrate of integrated circuits. These transistors are metal oxide based semiconductor devices that include source and drain regions with an insulated gate therebetween. As the density and performance of integrated circuits increase, the size of transistors must decrease. As a result, the thickness of the insulating gate dielectric layer must be made smaller. As for the gate dielectric, a desirable property of the dielectric layer is that it couples the upper gate electrode to the underlying channel so that the channel can respond to stimuli applied to the gate. In this sense, it is desirable for the dielectric to have a high dielectric constant, also known as high K. Silicon dioxide has been by far the most commonly used and effective gate insulator in the manufacture of integrated circuits. This has a very high level of integration and, in particular, can be manufactured with a very low defect density. As a result, silicon dioxide operates very efficiently, allowing these devices to have low leakage currents. Unfortunately, as the thickness of the gate dielectric decreases, the leakage current increases greatly. For example, thickness less than 20 SiO 2 leads to unacceptable leakage current and degraded device performance. Therefore, there is a need to replace SiO2 in CMOS devices. By having a thicker high-K layer with a reduced equivalent ( SiO2 ) oxide thickness, leakage current can be reduced.
对于高K电介质是理想的特性之一是,它是无定形的。它必须在整个使用寿命内保持为无定形的,包括制造期间以及随后的作为制成的集成电路一部分的功能运行期间。许多可选高K电介质具有足够高的K以及淀积时的足够集成度,但是在随后的处理步骤以及与之相关的加热之后,结果是这些膜会结晶。这样结晶的这些膜在它们的整个长度和宽度上结晶并不理想,而是在形成的晶体结构之间具有称为晶界的区域。这些晶界是出现泄漏以及影响电气性能的其它问题的区域。One of the properties that are desirable for a high-k dielectric is that it is amorphous. It must remain amorphous throughout its useful life, including during fabrication and subsequent functional operation as part of the finished integrated circuit. Many alternative high-K dielectrics have sufficiently high K and sufficient integration when deposited, but after subsequent processing steps and the heating associated therewith, the result is that these films crystallize. These films so crystallized are not ideally crystallized across their entire length and width, but instead have regions called grain boundaries between the crystal structures that form. These grain boundaries are areas where leakage and other problems affecting electrical performance occur.
当前,人们在开发具有比二氧化硅更高的介电常数的高K电介质上付出了许多努力。这样的高K电介质有很多,但是二氧化硅的一个优点是,它具有高带隙以及与硅的低界面态密度,这使得它成为一种非常有效的绝缘物。因此,已经发现为高K目的而开发的许多材料存在问题,因为它们没有足够高的带隙,或者因为它们难以制造成具有足够的集成度来防止通过电介质的漏电流。也还有一些尚未解决的问题,比如硅衬底和栅电极的热稳定性,氧化物/金属界面处的费米能级钉扎,以及尺度缩小。即使正在调查研究包括基于Hr和基于Zr的氧化物的无定形材料,但是仍然没有明确的解决方案,这是由于当集成到CMOS工艺流程中时这些材料会出现未解决的问题。另外,在制造过程的高温步骤中,这些材料会再结晶。基于La的氧化物材料可能能够用作Si CMOS器件的高K电介质。这种氧化物具有比SiO2高的介电常数,并且和硅接触时预期具有热动稳定性。Currently, many efforts are being made to develop high-K dielectrics with higher dielectric constants than silicon dioxide. There are many such high-k dielectrics, but one advantage of silicon dioxide is that it has a high band gap and low interface state density with silicon, making it a very effective insulator. Consequently, many materials developed for high-K purposes have been found to be problematic because they do not have a sufficiently high bandgap, or because they are difficult to fabricate with sufficient integration to prevent leakage current through the dielectric. There are also some unresolved issues, such as thermal stability of the silicon substrate and gate electrode, Fermi level pinning at the oxide/metal interface, and scaling down. Even though amorphous materials including Hr-based and Zr-based oxides are being investigated, there is still no clear solution due to unresolved issues with these materials when integrated into a CMOS process flow. Additionally, these materials recrystallize during the high-temperature steps of the manufacturing process. La-based oxide materials may be able to be used as high-K dielectrics for Si CMOS devices. This oxide has a higher dielectric constant than SiO2 and is expected to be thermodynamically stable in contact with silicon.
对于无定形的替代是单晶膜。理论上,高K介电膜能够通常由单晶体制成,虽然存在一些困难。困难之一就是匹配膜的晶体结构和下面的半导体的晶体结构,该半导体通常是硅,以及在成形过程期间,其中该成形过程实际上被极好形成。外延层在业内是公知的,这些外延层是单晶体构成的层。硅能够被外延制造。将非常薄的膜放置成单晶形式的技术之一是分子束外延。即使利用MBE技术,仍然难以确保获得无缺陷膜。An alternative to amorphous are single crystal films. In theory, high-K dielectric films can usually be made of single crystals, although there are some difficulties. One of the difficulties is matching the crystal structure of the film to that of the underlying semiconductor, typically silicon, and during the forming process, which is actually extremely well formed. Epitaxial layers are well known in the art, and these epitaxial layers are layers composed of single crystals. Silicon can be produced epitaxially. One of the techniques for placing very thin films into single crystal form is molecular beam epitaxy. Even with MBE technology, it is still difficult to ensure a defect-free film.
在开发新的高K电介质中,存在另一个潜在问题,即具有太高的介电常数。如果介电常数过高,会出现一种成为边缘场效应的效应,这种效应不利地影响晶体管的性能。这必须在栅极和源极/漏极之间进行过度耦合。因此,希望正在开发的材料具有通常在20到40之间的介电常数范围。随着技术进一步进步,该范围会有一些变化。Another potential problem in developing new high-K dielectrics is having a dielectric constant that is too high. If the dielectric constant is too high, an effect known as the fringe field effect occurs, which adversely affects the performance of the transistor. This must be overcoupled between gate and source/drain. Therefore, it is desirable that the materials being developed have a dielectric constant range of typically between 20 and 40. The range is subject to some changes as the technology advances further.
理想的高K电介质的另一个方面是关于其相当于某一厚的度氧化硅的等价电容。氧化硅已经是这么普遍和有效的被使用,以致于它已经变成了一种标准,该工业领域通常参照和氧化硅之间的关系来描述某种特性。在这种情况下,典型的理想氧化硅等价厚度是在5到15埃之间,但是5到15埃的氧化硅具有泄漏、可靠性、生长率以及均匀性等问题。因此,当膜这样小时,在制造和使用方面会存在困难。理想的耦合是,电介质具有5到15埃的氧化硅等价厚度,但是实际厚度要更高一些。Another aspect of an ideal high-k dielectric concerns its equivalent capacitance to a certain thickness of silicon oxide. Silicon oxide has been used so commonly and effectively that it has become a standard, and the industry often refers to a relationship with silicon oxide to describe certain properties. In this case, a typical ideal silicon oxide equivalent thickness is between 5 and 15 angstroms, but 5 to 15 angstroms silicon oxide has problems with leakage, reliability, growth rate, and uniformity. Therefore, when the film is so small, there are difficulties in manufacture and use. Ideally for coupling, the dielectric has a silicon oxide equivalent thickness of 5 to 15 Angstroms, but actual thicknesses are higher.
已经开发出含有铝的高K介电膜,然而,人们都知道铝在硅基器件中会带来高界面态密度和降低的迁移率。High-K dielectric films containing aluminum have been developed, however, aluminum is known to lead to high interface state density and reduced mobility in silicon-based devices.
因此,需要一种这样的介电膜,其具有理想范围内的介电常数、能够高集成度制造、理想范围内的厚度、不会降低迁移率或导致高界面态密度、并且能够以某种制造工艺制造。Therefore, there is a need for a dielectric film that has a dielectric constant within a desirable range, can be fabricated at high levels of integration, has a thickness within a desirable range, does not reduce mobility or result in high interface state density, and can be fabricated in a certain Manufacturing process manufacturing.
发明内容 Contents of the invention
为了实现上述和其它目的和优点,公开了一种半导体结构和构造该半导体结构的方法,该方法包括:提供半导体衬底;在该半导体衬底上方提供包括镧、镥以及氧的介电层;以及在该介电层上方提供电极层。To achieve the foregoing and other objects and advantages, a semiconductor structure and method of constructing the semiconductor structure are disclosed, the method comprising: providing a semiconductor substrate; providing a dielectric layer comprising lanthanum, lutetium, and oxygen over the semiconductor substrate; And an electrode layer is provided over the dielectric layer.
附图说明 Description of drawings
通过下面结合附图的优选实施例的详细描述,本领域技术人员将容易理解本发明的前述以及其它进一步更多的具体目的和优点:Through the following detailed description in conjunction with the preferred embodiments of the accompanying drawings, those skilled in the art will easily understand the aforementioned and other further specific purposes and advantages of the present invention:
图1是根据本发明的第一实施例的集成电路的一部分的剖面图;1 is a cross-sectional view of a part of an integrated circuit according to a first embodiment of the present invention;
图2是根据本发明的第二实施例的集成电路的一部分的剖面图;2 is a cross-sectional view of a portion of an integrated circuit according to a second embodiment of the invention;
图3是根据本发明的第三实施例的集成电路的一部分的剖面图;3 is a cross-sectional view of a part of an integrated circuit according to a third embodiment of the present invention;
图4是根据本发明的第四实施例的集成电路的一部分的剖面图;4 is a cross-sectional view of a part of an integrated circuit according to a fourth embodiment of the present invention;
图5是根据本发明的第五实施例的集成电路的一部分的剖面图;5 is a cross-sectional view of a part of an integrated circuit according to a fifth embodiment of the present invention;
图6是根据本发明的第六实施例的集成电路的一部分的剖面图;6 is a cross-sectional view of a part of an integrated circuit according to a sixth embodiment of the present invention;
图7是在700摄氏度退火之后淀积在根据本发明的硅上的50LaLuO3层的透射电子显微照片;FIG. 7 is a 50 Å deposited on silicon according to the invention after annealing at 700 degrees Celsius. Transmission electron micrograph of LaLuO 3 layer;
图8示出根据本发明在200摄氏度淀积在硅上的LaLuO3层的50A的卢瑟福反向散射能谱;以及Figure 8 shows the Rutherford backscattering spectrum of 5OA of a layer of LaLuO3 deposited on silicon at 200 degrees Celsius according to the present invention; and
图9通过图表示出在200摄氏度淀积在硅上的50LaLuO3层的C-V曲线。Figure 9 graphically shows the 50 CV curves of LaLuO 3 layers.
具体实施方式 Detailed ways
下面的详细描述仅是一种示例性实施例,而不是用于限制本发明或限制本发明的应用和使用。更恰当说,下面的描述提供了用于实施本发明的示例性实施例的适宜阐述。可以对所述部件的功能和结构进行多种对所述实施例的改变,而不会脱离在附属权利要求中设定的本发明的范围。一种包括镧、镥以及氧的高K介电膜提供了一种替代二氧化硅的优越候选材料。它同时具有以下优点:具有理想范围的介电常数、能够在高温保持为无定形以及具有低泄漏。The following detailed description is an exemplary embodiment only and is not intended to limit the invention or limit the application and uses of the invention. Rather, the following description provides a suitable illustration of exemplary embodiments for implementing the invention. Various changes to the described embodiments may be made in the function and structure of the components described without departing from the scope of the invention as set forth in the appended claims. A high-K dielectric film comprising lanthanum, lutetium, and oxygen provides a superior candidate to replace silicon dioxide. It combines the advantages of having a desirable range of dielectric constants, being able to remain amorphous at high temperatures, and having low leakage.
如图1所示,示出了集成电路的一部分10,其具有半导体材料衬底12、介电膜14以及导电膜16。衬底12至少在其表面上具有半导体区域。未示出的下面部分可以也是半导体材料或者可以是通常用于SOI的绝缘材料。半导体材料的例子包括单晶硅以及砷化镓。在衬底12上面的是介电层14。在介电层14上面的是导电膜16,该导电膜作为栅电极。介电层14作为栅极绝缘体或者栅极电介质。在此示出为在和介电膜14界面的表面附近区域上的衬底12是晶体管的沟道。As shown in FIG. 1 , a
栅极电介质14包括镧镥氧化物,它是一种包括镧、镥和氧的化合物。化学式是LaLuO3,其中镧和镥的浓度相同。在铝添加到该介电化合物的例子中(目前所讨论的),该化学式是La(Al)xLu1-xO3,其中x>0。镧镥氧化物公开为具有大约25的介电常数,以及大于5eV的带隙。结果,在衬底14上成功淀积镧镥氧化物使得该材料适于栅极电介质应用,该衬底比如是硅衬底。
这里公开的栅极电介质14优选的通过分子束外延(MBE)来形成,其中各种元素从热源蒸发。此外,元素可以利用电子束淀积、原子层化学气相淀积(ALCVD)、物理气相淀积、有机金属化学气相淀积以及脉冲激光淀积来产生。优选方法是MBE,其可以准确控制层的形成,包括厚度,在这种情况下,该厚度不小于大约15埃,优选的在20到100埃范围内。当前集成电路技术中栅极导体16通常是多晶硅,但是也可以是其它导体,比如金属,该金属包括但不限于钨、氮化钛、氮化钽或者可用作栅极导体的任何导体。The
由MBE淀积的栅极电介质14在确保膜在无定形条件下淀积中也很有用。使用当前MBE技术,衬底12的表面被初始清洁以使得它没有自然的氧化硅层,或者可以出现氧化硅或氮氧化硅的薄层(当前所讨论的)。该公开内容预期,在淀积镧镥氧化物之前,衬底12的表面被清洁并被加热以去除杂质,从而通过维持该硅衬底和氧化硅界面来减小工艺步骤。按照规定,此外通过在UHV条件下加热或者通过使用Si助解吸附过程或者Sr助解吸附过程,可以在淀积镧镥氧化物之前热去除自然氧化物。在该例子中,清洁表面(在去除低K材料之后)增加了介电堆的电容并增加了使该设备缩小到更小尺寸的能力。在另一个替换实施例中,预期到在淀积镧镥氧化物之前,该自然氧化物可以被去除,被氧和氮处理的表面在衬底12的表面上形成氮氧化硅。在该表面上形成氮氧化硅使得在该衬底和栅极电介质14之间提供界面,其中该界面具有的介电常数高于和SiO2之间界面的介电常数。The
在淀积镧镥氧化物的MBE过程中,利用喷嘴或等离子源,氧分子被可控地引入反应室,在该反应室中可以使用活性氧原子种类。镧和镥以及氧的引入因此形成镧镥氧化物的单层作为介电层14,其位于衬底12上方。During the MBE process for depositing lanthanum-lutetium oxide, using a nozzle or a plasma source, oxygen molecules are controllably introduced into a reaction chamber where reactive oxygen species can be used. The introduction of lanthanum and lutetium together with oxygen thus forms a monolayer of lanthanum-lutetium oxide as
该镧镥氧化物有利于在优化介电系数的区域中具有低泄漏和较高电容。一些其它材料具有可识别的缺陷。例如,氧化镧的二元化合物具有适当范围内的介电常数,但是它吸水。吸水对于理想的集成电路制造是非常有害的。例如,氧化镧吸水会导致结构完整性问题,从而使得它不能用于形成集成电路结构。镥的引入可以提供一种非常稳定的栅极电介质,其保持无定形并在高温下不会再结晶,因此当它和衬底12接触时会保持稳定。此外,使用镧镥氧化物可以获得高带隙,其高于5eV,并具有合理的能带偏移、大约25的介电常数以及类似于硅的热膨胀系数。The lanthanum-lutetium oxide favors low leakage and high capacitance in the region of optimized dielectric coefficient. Some other materials have identifiable defects. For example, a binary compound of lanthanum oxide has a dielectric constant in the proper range, but it absorbs water. Water absorption is very detrimental to ideal IC fabrication. For example, water absorption by lanthanum oxide can cause structural integrity problems, making it unusable for forming integrated circuit structures. The introduction of lutetium can provide a very stable gate dielectric that remains amorphous and does not recrystallize at high temperatures, thus remaining stable when in contact with the
镧镥氧化物的另一个益处是,介电常数可以基于镧含量和镥含量的范围而变化。因此,可以获得大约10到25之间的最优化介电常数。当镧含量相对于镥含量变化时,甚至能够获得稍微有些大的系数,但是这会导致涉及吸水的问题。此外,该公开内容预期在介电层14中包含铝或氮,从而增加该介电层的稳定性、缺陷钝化以及可能会增加介电常数。Another benefit of lanthanum-lutetium oxide is that the dielectric constant can vary based on the range of lanthanum content and lutetium content. Therefore, an optimum dielectric constant of about 10 to 25 can be obtained. Even somewhat larger coefficients can be obtained when the lanthanum content is varied relative to the lutetium content, but this leads to problems related to water absorption. Furthermore, the disclosure contemplates the inclusion of aluminum or nitrogen in the
即使在高达1025摄氏度或者更高温度下该镧镥氧化物仍然有利的保持无定形性。1025摄氏度通常是当前制造工艺中的最高温度。因此,镧镥氧化物已经被发现能够承受集成电路处理中将会接收到的最高温度,并保持无定形性,其中集成电路处理由许多典型工艺构成,以获得最先进的几何图形。通常希望最高处理温度降下一些,但是最高温度仍将很可能保持相当高,因为源极/漏极中的搀杂剂激活需要高温,并且这种激活在可预知的未来仍是需要的。最高温度可以降低到稍微低于1025摄氏度,但是仍然在至少相当长的一段时间内高于900摄氏度。然而,温度将出现大幅度下降是不能确定的,而且1025摄氏度在相当一段时间仍持续是一个有效需要。因此,该无定形性镧镥氧化物获得了预期温度范围上的理想高K特性和高集成度。The lanthanum-lutetium oxide advantageously remains amorphous even at temperatures as high as 1025°C or higher. 1025 degrees Celsius is usually the highest temperature in current manufacturing processes. Consequently, lanthanum-lutetium oxide has been found to be able to withstand the highest temperatures it will receive in integrated circuit processing, which consists of many typical processes, to obtain state-of-the-art geometries, and to remain amorphous. It is generally expected that the maximum process temperature will be lowered somewhat, but the maximum temperature will still likely remain quite high because dopant activation in the source/drain requires high temperatures and such activation will still be required for the foreseeable future. The maximum temperature can be reduced to slightly below 1025 degrees Celsius, but still above 900 degrees Celsius for at least a considerable period of time. However, it is not certain that the temperature will drop significantly, and 1025 degrees Celsius is still a valid requirement for quite some time. Therefore, the amorphous lanthanum-lutetium oxide achieves desirable high-K characteristics and high integration over the expected temperature range.
能够淀积无定形镧镥氧化物的有效高K介电膜的另一个益处是,它能够不仅在硅上是非常有效的,而且在砷化镓上也是非常有效的。有效实施砷化镓CMOS技术从而利用其更高迁移率优点中存在的一个问题是,砷化镓中所用栅极电介质非常难以匹配硅的栅极电介质的集成度,其通过在高温生长硅氧化物而实现。因此,在大多数应用场合,已经证实硅优于砷化镓。现在利用使用MEB淀积的有效高K电介质,获得的结果是,不论是淀积在硅上,还是砷化镓或一些其它半导体材料上,栅极电介质都能够具有高集成度。从而可能砷化镓将成为大多数集成电路的优选选择,但是当前却仅是半导体市场的冰山一角。Another benefit of being able to deposit efficient high-K dielectric films of amorphous lanthanum-lutetium oxide is that it can be very effective not only on silicon but also on gallium arsenide. One of the problems in effectively implementing GaAs CMOS technology to take advantage of its higher mobility benefits is that the gate dielectric used in GaAs is very difficult to match the integration of the gate dielectric of silicon, which is obtained by growing silicon oxide at high temperature. And realize. Therefore, silicon has proven superior to gallium arsenide for most applications. Now with the efficient high-k dielectric deposited using MEB, the result is that the gate dielectric can have a high degree of integration whether deposited on silicon, gallium arsenide or some other semiconductor material. Gallium arsenide may thus become the preferred choice for most integrated circuits, but it is currently only the tip of the iceberg in the semiconductor market.
如图2所示,集成电路的一部分18包括一个衬底20、阻挡电介质22、高K电介质24以及导体26。在这种情况下,高K电介质24类似于或相似于图1中的膜14,因为它是镧镥氧化物。导体26相似于导体16,而衬底20相似于图1中的衬底12,其具有清洁表面、表面上的残余自然氧化物或者表面上存在的氮氧化物之一,如前所述。阻挡电介质22,其也可以被称为界面层,被选用作为绝缘体,因为其具有理想特性。例如,这可以是镧氧化物、镥氧化物、硅氧化物或者硅氮氧化物。阻挡电介质22的存在可以确保高K电介质24和阻挡电介质22的组合具有防止不必要电流的足够绝缘特性。例如,该组合可以具有高带隙并可以具有足够高的介电常数。特别是,这设置了一个高带隙材料直接接触衬底20,该衬底是电子注入的势源。阻挡电介质22的另一个潜在利用是,如果选为衬底20的材料存在问题或者和镧镥氧化物发生反应,那么可以将其作为扩散势垒区。As shown in FIG. 2 , a
如图3所示,示出集成电路的一部分28,其包括衬底30、介电膜32以及导体34。在这种情况下,衬底30相似于衬底20和12,导体34相似于导体26和16。介电膜32替代电介质14以及电介质22和24的组合。在这种情况下,介电膜32具有渐次变化浓度的镧或镥,这意味着,二元材料,也就是镧氧化物或镥氧化物,靠近衬底30以及介电膜32的界面形成,并渐变为三元材料,也就是镧镥氧化物,通过添加镧或者镥而形成为和导体24交界的层。在介电膜32中,靠近和衬底30的界面,该材料实质上是纯镧氧化物或镥氧化物。在向导体34移动的过程中,在镧氧化物靠近衬底30的界面淀积的情况下,镥的浓度连续增加,直到在靠近和导体34之间界面处介电膜32中的镧和镥之间的比率是1比1。该方法的优点是,在最靠近衬底30处获得理想的高带隙,并且避免在镧氧化物或镥氧化物和镧镥氧化物之间产生任何突变界面。获得的介电常数也可以通过控制浓度增加的速率来进行调节,也就是镧和镥之间的1比1的比率可以在和导体34交界之前很好的实现。一种可选方案是继续渐次变化,以超过1比1的比率,从而镧的浓度超过镥的浓度,反之亦然。As shown in FIG. 3 , a
如图4所示,示出集成电路的一部分36,其包括衬底40、阻挡电介质42、高K电介质44、阻挡电介质46以及导体48。在这种情况下,衬底40相似于衬底12、20以及30。阻挡电介质42相似于阻挡电介质22。高K电介质44相似于高K电介质14和24。导体48相似于导体16、26以及34。阻挡层46在高K电介质44和导体48之间进行阻挡。阻挡体46用于导体48和高K电介质44之间具有相容性问题的场合。阻挡体46也很可能从镧氧化物、镥氧化物、硅氧化物以及硅氮氧化物中进行选择。阻挡电介质46的目的是在导体48和高K电介质44之间提供扩散势垒区。当然,希望阻挡层46具有高介电常数,但是其目的是防止导体48和高K电介质44之间出现问题。优选选择很可能是镧氧化物或镥氧化物,因为它们具有比硅氧化物更高的介电常数。As shown in FIG. 4 , a
如图5所示,示出集成电路的一部分50,其包括导体52、高K电介质54以及导体56。在这种情况下,高K电介质应用于两个导体之间。这主要出现在导体52是用于存储电荷的浮栅的情况。它还能够出现在52和56包括用于存储电荷的电容板的场合。一种这样的例子是动态随机存取存储器的存储单元。在这种情况下,还希望高K电介质54具有高介电常数以及具有低泄漏的理想特性。As shown in FIG. 5 , a
如图5所示,高K电介质54是具有渐次变化浓度的镧镥氧化物。镧的浓度在中间最大,而在和导体52和导体56的界面处是纯或几乎纯的镥氧化物。这就提供了比较高的介电常数,并且在和导体52以及导体56的界面处提供高带隙,从而它既是一种高K电介质又是优良的绝缘体。通过使高K电介质54渐次变化,避免了绝缘体类型之间出现明显的分界面。材料类型之间的突变往往是电荷能够被捕获的地方。利用渐次变化浓度,避免了突变的界面。在晶体管的情况,仅在靠近衬底的位置具有高带隙是非常重要的,因为那是可能注入电荷的地方,而在部分50的情况,电荷能够从导体52或者导体56注入。因此,希望在和导体52以及导体56的界面处具有高带隙。应当理解的是,本公开内容预期到反向材料堆栈,也就是,其中镧的浓度在中间最大,而在和导体56以及导体52的界面处是纯或几乎纯的镥氧化物。As shown in FIG. 5, the high-
如图6所示,示出集成电路的一部分60,其包括导体62、阻挡电介质64、高K电介质66、阻挡电介质68以及导体70。这是相似于图5的结构。导体62相似于导体52,导体70相似于导体56,层64、66以及68的组合相似于图5中的高K电介质54。在图6的情况下,介电层64和68都用于提供高带隙以及在导体62和70以及高K电介质66之间作为扩散势垒区。因此,对于获得足够绝缘质量以及提供扩散势垒区给高K电介质66,增加阻挡层64和68是必要的。导体62和70可以具有不同特性。一个可以是多晶硅。另一个可以是一种金属,在这种情况下,阻挡电介质的类型希望是不同的。高K电介质66包括镧镥氧化物,其具有如图1-5的结构中的膜用到的镧镥氧化物所述的那些益处。As shown in FIG. 6 , a
不同于晶体管的形成在两个导体的情况下将需要阻挡体的可能性会增加,因为,实际上它适合用于某些情况下在导体62和70之间进行注入。因此,需要阻挡体64和68或者如图5那样渐次变化的可能性更可能成为实际发生的情况,其中上述需要阻挡体64和68或者如图5那样渐次变化会导致这种注入在不想要它发生的时候不发生。因此,需要阻挡体64和68或者如图5那样渐次变化的可能性在通过注入进行电荷存储的情况下较大。以及,在它纯粹作为电容的情况下,仍然更可能需要阻挡层64和68。电容的主要目的是存储电荷,从而在和导体之间界面处具有高带隙的重要性甚至大于晶体管的重要性。The likelihood that a barrier would be required in the case of two conductors other than the formation of a transistor increases because, in fact, it is suitable for implantation between conductors 62 and 70 in some cases. Therefore, the possibility of requiring barriers 64 and 68 or a gradual change as in FIG. 5 is more likely to be a practical occurrence, wherein the above-mentioned need for barriers 64 and 68 or a gradual change as in FIG. When it happens it doesn't happen. Therefore, the need for barriers 64 and 68 or the possibility of gradation as in FIG. 5 is greater in the case of charge storage by injection. And, in the case where it acts purely as a capacitor, barrier layers 64 and 68 are still more likely to be needed. The main purpose of a capacitor is to store charge, so having a high bandgap at the interface with a conductor is even more important than a transistor.
下面的例子示出了根据本发明的一个实施例的一种用于构建图1中所示半导体结构比如结构10的方法。该方法通过提供单晶半导体衬底来开始,该衬底包括选自元素周期表族IV或族III-V的材料。根据本发明的优选实施例,半导体衬底是具有(100)定向的硅片。至少一部分半导体衬底具有裸露面,而下面所述的衬底的其它部分会包括其它结构。文中的术语“裸露”表示衬底的该部分中的表面已经被清洁以去除任何氧化物、杂质或者其它外来材料。众所周知,裸露硅是高反应性的,容易形成一个自然氧化物。术语“裸露”的意思中包括这样一种自然氧化物。下面的过程优选的通过分子束外延(MBE)来执行,但是根据本发明也可以使用其它淀积过程,比如,物理气相淀积、原子层淀积或者有机金属化学气相淀积。通过在MBE室中加热该衬底到高于800摄氏度的温度来去除该自然氧化物。清洁的硅表面显示(2×1)表面重构,其由反射高能电子衍射(RHEED)监测到。在另一个实施例中,通过在MBE装置中淀积锶、钡、锶和钡的组合、或者其它碱土金属或碱土金属的组合的薄层(优选1-3个单层)并将其加热到超过750摄氏度的温度,从而去除该自然氧化物。The following example illustrates a method for constructing a semiconductor structure such as
紧接该明显的(2×1)表面重构的出现,衬底的温度降低到室温和500摄氏度之间,优选的是50到400摄氏度之间。然后氧气引入该MBE室,直接朝向被清洁衬底。同时,喷发源上的阀门被打开,使得镧和镥的原子撞击到半导体衬底上,形成镧镥氧化物的层14。在另一个实施例中,可以引入铝来形成镧铝镥氧化物层。接着淀积层14到所需厚度,通过物理气相淀积或者其它本领域公知的淀积技术来淀积栅极电极。Immediately after the appearance of this pronounced (2x1) surface reconstruction, the temperature of the substrate is lowered to between room temperature and 500 degrees Celsius, preferably between 50 and 400 degrees Celsius. Oxygen is then introduced into the MBE chamber, directed towards the substrate being cleaned. Simultaneously, the valve on the eruption source is opened, so that atoms of lanthanum and lutetium impinge on the semiconductor substrate, forming a
如图7所示,示出在200摄氏度淀积在硅上的50厚的LaLuO3层的透射电子显微照片80。如图所示,在构建该介电层之后,淀积TaN层并将其在700摄氏度退火。在该介电层和该衬底之间的界面极其平整,并且出现薄的界面层。将该层加热到900摄氏度不会引发任何的再结晶。As shown in Figure 7, a 50 Transmission electron micrograph of a thick LaLuO3 layer80 . As shown, after building up the dielectric layer, a TaN layer is deposited and annealed at 700 degrees Celsius. The interface between the dielectric layer and the substrate is extremely smooth and a thin interfacial layer occurs. Heating the layer to 900 degrees Celsius did not induce any recrystallization.
图8示出淀积在硅上的LaLuO3介电层的RBS能谱90,示出了镧和镥的存在。能谱分析显示出镧和镥的比率接近1∶1。通过参照施加电压构建电容器和测量电容量,确定该氧化物层的电特性。图9示出了电容的电容量-电压曲线100,示出了性能良好的特性,其中该电容利用硅上的LaLuO3介电层来构建。Figure 8 shows the
根据本发明的另一个实施例,在图1的结构10中,硅衬底可以覆盖有热生长的二氧化硅层(未示出)。或者,硅的表面可以覆盖有氮氧化硅层。可以利用化学方法来制备该二氧化硅,该方法留下不超过10埃的氧化物。或者,硅衬底可以在上述情况中被原位清洁,以留下一个清洁的、重构良好的表面。然后该表面暴露到氧流中,该氧流是氧分子、等离子源中产生的活性氧或者臭氧的形式。可以控制该暴露条件,以便获得1到15埃、优选3-8埃的二氧化硅的理想厚度范围。在另一个实施例中,清洁的硅表面可以暴露到氧流和氮流中,以形成氮氧化硅层。氮可以以气态形式施加,包括一氧化二氮或离子源中产生的活性氮。在制备二氧化硅或氮氧化硅的界面层之后,可以淀积高K介电层。According to another embodiment of the invention, in the
根据本发明的另一个实施例,该高K电介质可以是La(Al)xLu1-xO3Ny的形式,其中y>0。这可以通过上述的在存在氮的情况下淀积高K介电层来实现。氮结合到高K介电膜中能够潜在的增加热稳定性以及减小陷阱密度。According to another embodiment of the present invention , the high-K dielectric may be in the form of La(Al) xLu1 - xO3Ny , where y>0. This can be accomplished by depositing a high-K dielectric layer in the presence of nitrogen as described above. Nitrogen incorporation into high-K dielectric films can potentially increase thermal stability and reduce trap density.
虽然本发明已经在多个实施例中描述,但是还存在可以结合利用的其它实施例和其它材料,其将提供益处或者和本发明相关的一些益处。可以使用不同于上述材料的其它材料。此外,还可以添加一些材料到镧镥氧化物中,可以获得除了组合中镧镥氧化物以及所述多种浓度所提供的益处之外的其它益处。因此,由权利要求来限定本发明的范围。While the invention has been described in a number of embodiments, there are other embodiments and other materials that may be utilized in conjunction that will provide benefits or some benefits related to the present invention. Other materials than those described above may be used. Additionally, materials may be added to the lanthanum-lutetium oxide that may provide additional benefits beyond those provided by the lanthanum-lutetium oxide in combination and the various concentrations described. Accordingly, the scope of the present invention is defined by the appended claims.
Claims (4)
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