TWI308376B - Method for making a semiconductor device including shallow trench isolation (sti) regions with a superlattice therebetween - Google Patents
Method for making a semiconductor device including shallow trench isolation (sti) regions with a superlattice therebetween Download PDFInfo
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- TWI308376B TWI308376B TW095122068A TW95122068A TWI308376B TW I308376 B TWI308376 B TW I308376B TW 095122068 A TW095122068 A TW 095122068A TW 95122068 A TW95122068 A TW 95122068A TW I308376 B TWI308376 B TW I308376B
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/60—Insulated-gate field-effect transistors [IGFET]
- H10D30/601—Insulated-gate field-effect transistors [IGFET] having lightly-doped drain or source extensions, e.g. LDD IGFETs or DDD IGFETs
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/80—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
- H10D62/81—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation
- H10D62/815—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW]
- H10D62/8161—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW] potential variation due to variations in composition or crystallinity, e.g. heterojunction superlattices
- H10D62/8162—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW] potential variation due to variations in composition or crystallinity, e.g. heterojunction superlattices having quantum effects only in the vertical direction, i.e. layered structures having quantum effects solely resulting from vertical potential variation
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
- H10D84/0123—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs
- H10D84/0126—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs
- H10D84/0165—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs the components including complementary IGFETs, e.g. CMOS devices
- H10D84/0167—Manufacturing their channels
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- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
- H10D84/0123—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs
- H10D84/0126—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs
- H10D84/0165—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs the components including complementary IGFETs, e.g. CMOS devices
- H10D84/0188—Manufacturing their isolation regions
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
- H10D84/02—Manufacture or treatment characterised by using material-based technologies
- H10D84/03—Manufacture or treatment characterised by using material-based technologies using Group IV technology, e.g. silicon technology or silicon-carbide [SiC] technology
- H10D84/038—Manufacture or treatment characterised by using material-based technologies using Group IV technology, e.g. silicon technology or silicon-carbide [SiC] technology using silicon technology, e.g. SiGe
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- H10W10/17—
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- Insulated Gate Type Field-Effect Transistor (AREA)
- Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)
- Element Separation (AREA)
Description
'1308376 41 側壁隔絕層 42 環狀植入物區 43 環狀植入物區 80 STI區 82 非早晶枪條 83 非早晶析條 八、本案I有化學式時,請揭示最能齡發明特徵的化學式: 九、發明說明: 【相關申請案】 本申睛案係主張2005年6月2〇日提出之美國專利申請臨時案 (provisional application)第6〇/692 1〇1號之優先,而且本申請案係^ ^004年11月18日提出之美國專利申請第1〇/992,422號之部份連續申 凊案(Contmuation-m-part appiicati〇n),美國專剌申請第 1〇/992 422 號 係為2003年8月22日提出之美國專利申請第腦47,_號,現為美 國專利第6,958,伽號之部份連續_請案,美國專利第6,958,486號^ 為2003年6月26日提出之美國專利申請第1〇/6〇3,696號及第 10/603,621號_請案之部份連射請案,上述各巾請案之 内容在此列為本發明之參考資料 【發明所屬之技術領域】 本發明係有關半導體之領域,且特別是有關於以能帶工程(energy bgnd engineering)為基礎而具有增進特性之半導體及其相關之方法。 【先前技術】 利用諸如增強電荷載體(charge carriers)之動性(mobility),以便增進半 導體元件性能之相關構造及技術,已多有人提出。例如,Curr^等人 之美國專利申請第2003/0057416號案中揭示了矽、石夕_錯 (silicon-germanium)、以及釋力矽(relaxed silicon)與包括原本將會導致 1308376 性能劣退的無雜質區(impurity-free zones)等的形變材質層(strained material layers)。其在上矽層中所形成的雙軸向形變(biaxiai strain)改變 了載體的動性,並得以製作較高速與/或較低功率的元件。Fitzgerald 等人的美國專利申請公告第2003/0034529號案中則揭示了同樣亦以 類似的开> 變石夕技術(strained siiicon technology)為基礎的一種CMOS反 向器(CMOS invertei^。'1308376 41 Sidewall insulation layer 42 Annular implant zone 43 Annular implant zone 80 STI zone 82 Non-early grain bar 83 Non-early crystallized strips 8. When the case I has a chemical formula, please reveal the characteristics of the most inventive invention. Chemical Formula: IX. Invention Description: [Related Applications] This application is a priority of the US Patent Application Provisional Application No. 6/692 1〇1, which was filed on June 2, 2005, and This application is a part of the continuous application (Contmuation-m-part appiicati〇n) of U.S. Patent Application No. 1/992,422, filed on November 18, 2005, U.S. Patent Application No. 1/992 422 is the United States patent application No. 47, _, filed on August 22, 2003, and is now U.S. Patent No. 6,958, part of the gamma continuous _ request, US Patent No. 6,958, 486 ^ for June 2003 U.S. Patent Application Serial No. 1/6〇3,696 and No. 10/603,621, filed on the 26th, the contents of the above-mentioned claims are listed as references in the present invention. TECHNICAL FIELD The present invention relates to the field of semiconductors, and in particular to With engineering (energy bgnd engineering) has based its method of enhancing semiconductor characteristics related to the. [Prior Art] Various constructs and techniques such as enhancing the mobility of charge carriers to enhance the performance of semiconductor elements have been proposed. For example, in the case of US Patent Application No. 2003/0057416 to Curr et al., it is disclosed that silicon germanium, silicon-germanium, and relaxed silicon and including originally would cause 1308376 performance degradation. Strained material layers such as imperative-free zones. The biasiasi strain formed in the upper layer changes the mobility of the carrier and enables the fabrication of higher speed and/or lower power components. U.S. Patent Application Publication No. 2003/0034529 to Fitzgerald et al. discloses a CMOS inverter (CMOS invertei^) which is also based on a similarly-strained siiicon technology.
Takagi的第6,472,685 B2號美國專利中揭示了一種半導體元件,包含 有夾在石夕層之間的一層石夕及碳層,以使其第二石夕層的傳導能帶 (conduction band)及鍵結能帶(valence band)承受伸張形變(tensiie strain)。具有較小等效質量(effective mass)並由施加於閘電極上的電場 所誘發的電子,便會被限制在其第二矽層内,因此即可認定其n通道 MOSFET得以具有較高的動性。U.S. Patent No. 6,472,685, issued to U.S. Patent No. 6, 472,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, The valence band is subjected to a tensiie strain. An electron with a small effective mass and induced by an electric field applied to the gate electrode is confined to its second layer, so that its n-channel MOSFET can be considered to have a higher dynamic Sex.
Ishibashi等人的第4,937,204號美國專利中揭示了一種超晶格,其中 包含一整層的或部份層的雙元化合物c〇mp〇imd)的半導體^層多 層(少於八個單層(mon〇layer))構造,係交替地以磊晶成長(epitaxial g〇Wth)的方式增長而成。其主電流流動方向係垂直於超晶格中的各層U.S. Patent No. 4,937,204 to the disclosure of U.S. Patent No. 4,937, issued to the entire entire entire entire entire entire entire entire entire entire The mon〇layer)) structure is grown alternately in the form of epitaxial g〇Wth. The main current flow direction is perpendicular to the layers in the superlattice
Wang等人的第5,357,119號美國專利中揭示了 si-Ge的一種短週期超 晶格(short period superlattice),利用減低超晶格中的合金散佈(all〇y scattering)而達成其較高的動性。依據類似的原理,Canddaria的美國 第5,683,943號專利中揭示了一種增進動性之m〇sfeT,其包含一通 道層(charnel layer),該通道層包括有矽合金與第二種物質,此第二種 物質於梦晶格暢替代性地出現,其成分百分比係能使通道層處於伸 張應力(tensile stress)之狀態。A short period superlattice of si-Ge is disclosed in US Patent No. 5,357,119 to Wang et al., which is achieved by reducing the alloy scattering in the superlattice (all〇y scattering). Motivation. In accordance with a similar principle, U.S. Patent No. 5,683,943 to the disclosure of U.S. Pat. The substance appears alternately in the dream crystal, and the percentage of the composition is such that the channel layer is in a state of tensile stress.
Tsu的第5,216,262號美國專利中揭示了一種量子井(qua咖構 造,其包含有兩個屏蔽區(barrier region)以及夾在屏蔽區之間的一薄的 蠢晶長成半導體層。其每-屏蔽區各係由厚度範圍大致在二至六個交 疊的Si02/Si單層所構成。屏蔽區之間亦另夾有更厚的石夕材質區 (section)。 屬年9 j 6日線上發行的顧物理及材料科學及製程(Applied 1308376U.S. Patent No. 5,216,262 to the disclosure of U.S. Patent No. 5,216,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, Each of the shielding zones consists of a single layer of SiO 2 /Si with a thickness ranging from approximately two to six. A thicker section of the Shi Xi material is also sandwiched between the shielding zones. Issued by Physic and Materials Science and Process (Applied 1308376
Physics and Materials Science & Processing)391 - 402 頁,一篇題為「石夕 質奈米構造元件中之現象」(“Phenomena in silicon nanostructure devices”)的文章中,Tsu揭示了一種矽及氧的半導體-原子超晶格 (semiconductor-atomic superlattice,SAS)〇 此 Si/O 超晶格構造被揭露為 一種有用的矽量子及發光元件。其中特別揭示了如何製作並測試一種 綠色電輝光二極體(electroluminescence diode)的構造。該二極體構造.中 的電流流動方向是垂直的,亦即,垂直於SAS的層面。該文中所揭 示的SAS可以包含半導體層,半導體層之間係由諸如氧原子及c〇分 子等被吸收的物質(adsorbedspecies)所分離開。被吸收的氧單層以外 所長成的矽,被描述為磊晶層,其具有相當低的缺陪密度(defect density)。其中的一種SAS構造包含有一 Unm厚度的矽質部份,其 係約為八個矽原子層,而其另一種構造中的矽質部份的厚度則有其述 厚度的兩倍_。物理評論通訊(Physics Review Letters),Vol. 89, No. 7 (2002年8月12日)中,Luo等人所發表的一篇題為「直接間隙發光矽 之化學設計」(“Chemical Design of Direct-Gap Light-Emitting Silicon”) 的文章’更進一步地討論了 Tsu的發光SAS構造。Physics and Materials Science &Processing; 391 - 402, in an article entitled "Phenomena in silicon nanostructure devices", Tsu reveals a kind of helium and oxygen. Semiconductor-atomic superlattice (SAS), a Si/O superlattice structure, has been unveiled as a useful quantum and luminescent element. It specifically reveals how to fabricate and test the construction of a green electroluminescence diode. The direction of current flow in the diode structure is vertical, that is, perpendicular to the level of the SAS. The SAS disclosed herein may comprise a semiconductor layer separated by adsorbed species such as oxygen atoms and c〇 molecules. The ruthenium formed outside of the absorbed oxygen monolayer is described as an epitaxial layer which has a relatively low defect density. One of the SAS structures comprises an enamel portion having a thickness of Unm which is about eight layers of germanium atoms, and the thickness of the tannin portion of the other structure is twice as thick as the thickness. Physics Review Letters, Vol. 89, No. 7 (August 12, 2002), published by Luo et al., entitled "Chemical Design of Direct Gap Luminescence" ("Chemical Design of The article "Direct-Gap Light-Emitting Silicon") further discusses the luminescent SAS construction of Tsu.
Wang、Tsu及Lofgren等人的國際申請公報WO 02/103,767 A1號案中 揭示了薄矽及氧,礙,氮,填,娣,砷或氫的一種屏蔽建構區塊,其 可以將垂直流經晶格的電流減小超過四個十之次方冪次尺度(f〇ur orders of magnitude)。其絕緣層/屏蔽層可容許在鄰接著絕緣層之處沉 積有低缺陷度的蟲晶石夕。A shield construction block of thin tantalum and oxygen, nitrogen, nitrogen, fill, helium, arsenic or hydrogen is disclosed in the International Application Publication No. WO 02/103,767 A1 to Wang, Tsu, and Lofgren et al. The current of the crystal lattice is reduced by more than four tenth power orders (f〇ur orders of magnitude). The insulating layer/shield layer allows for the deposition of low-defect fibrites adjacent to the insulating layer.
Mears等人在已公告的英國專利申請第2,347,52〇號案中揭示,非週期 性光子能帶間隙的原理構造(aperiodic photonic band-gap, APBG)可應 用於電子此帶間隙工程(electronic bandgap engineering)之中。特別是, 該申请案中揭示’材料參數(materialparameters),例如,能帶最小值 的位置,等效質量,等等,皆可加以調節,以便獲致具有所要能帶構 造的特性之新的非週期性材料。其他的參數,諸如導電性(electrical conductivity),熱傳導性(thermal conductivity)及介電係數(didectric permittivity)或導磁係數(magneticpermeability),皆被宣稱亦可能被設 计於材料之中。 【發明内容】 1308376 一種製作一半導體元件之方法’可包含形成複數淺溝渠隔離(STI)區於 一半導體底材中。再者,可沉積複數層覆蓋該底材,以定義覆蓋該底 材分別介於鄰接STI區之間的超晶格,並定義分別覆蓋STI區之非__ 晶區(non-monocrystalline regions)。該方法可更包含利用至少—主動區 (activearea,AA)遮罩選擇性地移除該非單晶區之至少一部份。 °° 尤其是,該方法可更包含形成複數個與該些超晶格聯結的與 PMOS電晶體通道,以使得該半導體元件包含一 CM〇s半導體元件。 再者,選擇性地移除可包含圖案化具有至少一AA遮罩之一光阻屉,Mears et al., in the published British Patent Application No. 2,347,52, discloses that aperiodic photonic band-gap (APBG) can be applied to electronic bandgap engineering. In engineering). In particular, the application discloses that 'material parameters, for example, the position of the band minimum, the equivalent mass, etc., can be adjusted to achieve a new aperiodic characteristic of the desired band structure. Sexual material. Other parameters, such as electrical conductivity, thermal conductivity, and didectric permittivity or magnetic permeability, are all claimed to be also designed into the material. SUMMARY OF THE INVENTION 1308376 A method of fabricating a semiconductor device can include forming a plurality of shallow trench isolation (STI) regions in a semiconductor substrate. Further, a plurality of layers may be deposited to cover the substrate to define a superlattice covering the substrate between adjacent STI regions, and defining non-monocrystalline regions covering the STI regions, respectively. The method can further include selectively removing at least a portion of the non-single crystal region using at least an active area (AA) mask. In particular, the method can further include forming a plurality of PMOS transistor channels coupled to the superlattices such that the semiconductor component comprises a CM 〇 semiconductor component. Further, selectively removing the photoresist that can include patterning at least one AA mask,
^外,該至少-AA鮮可以是-單—基線μ遮罩。在其他實施例 中,該至少-AA遮罩可包含用於舰〇s電晶體之一第一過大的通 道阻,(firSt〇versizedChannd-St〇P)AA 遮罩,以及用於PM0S 電晶體 之-第二過大的通道阻絕AA遮罩。因此,該方法更可包含利用該 厂過大的通道阻絕AA遮罩,進行一第一通道阻絕植入,利用該 過大的通道阻絕AA遮罩進行-第二通道阻絕棺入。f谁一舟而令,In addition, the at least -AA fresh can be a - single-baseline μ mask. In other embodiments, the at least -AA mask may comprise a first oversized channel resistance for one of the ship's s transistors, a (firSt〇versizedChannd-St〇P) AA mask, and for a PMOS transistor. - The second oversized channel blocks the AA mask. Therefore, the method may further comprise: using a large channel of the factory to block the AA mask, performing a first channel blocking implant, and using the excessive channel to block the AA mask - the second channel blocks the intrusion. f who is a boat,
一非半導體單層。此外,該至少一非 的基底半導體部份的一晶禮晶格内。 在某些實施例中,該至少一非丰蓽稱A non-semiconductor monolayer. Further, the at least one non-base semiconductor portion is within a crystal lattice. In some embodiments, the at least one non-rich name
非半導體單層可為一單一單層厚度。此 皆小於8個單層的厚度。該超晶格於一最 的基底半導體部份可皆為相同數目單層之厚度The non-semiconductor monolayer can be a single single layer thickness. These are all less than the thickness of 8 single layers. The superlattice may be the same number of single layer thicknesses in one of the most base semiconductor portions
盍層。在某些實施例中,所有 之厚度,而在其他實施例中, 單層之厚度。另外,所有的基 7 '1308376 半1來說’每一基底半導體部份可各包含有由IV族半導體,III-V族 導’以及II-VI族半導體等所組成的群組之中所選定的一基底半 t 同樣舉例來說,每一非半導體層可各包含由氧、氮、氟及碳_ 乳所構成之群組中所選定的一非半導體。 【實施方式】盍 layer. In some embodiments, all thicknesses, and in other embodiments, the thickness of the single layer. In addition, all of the base 7 '1308376 half 1 'each of the base semiconductor portions may each include a group consisting of a group IV semiconductor, a group III-V conductor, and a group II-VI semiconductor. Similarly, for example, each of the non-semiconductor layers may each comprise a non-semiconductor selected from the group consisting of oxygen, nitrogen, fluorine, and carbon-milk. [Embodiment]
本發明說明書所附圖式,後面的說明文字段落之中將詳細說明本 天明,而圖式之中所顯示的係為本發明之較佳實施例。不過,本發明 仍可以許多種不同的形式實地施行,因此本發明之範疇當然不應限定 於圖式中所顯示之實施例上。相對地,此些實施例僅是被提供來使本 發明所揭示之發明内容更為完整詳盡,並得使習於本技藝者能夠完全 地,,本發明之範疇。在本發明的整篇說明文字之中,相同的圖式參 考才示號係用以標示相同或相當的元件,而加撇②rime)或多重加撇符號 則係用以標示不同實施例中的類似元件。 本發明係相關於在原子或分子的層級上控制半導體材料的特性,以達 成增進半導體元件之性能。此外,本發明亦係有關於增進材料的辨 別、創造以及使用,以便將其應用於半導體元件的導電路徑之中。 本案申請人所提之理論顯示,本發明此地所揭示描述的某些超晶格構 造,可以降低電荷載體的等效質量,並藉由於此種降低可導致較高的 電荷載體動性,但申請人同時聲明本發明之範疇不應限定於此理論 上。本發明所屬技藝領域内的文獻之中,對於等效質量有多種定義加 以描述說明。作為等效質量上之增進的一種量測尺度,申請人使用「導 電性反等效質量張量」(“conductivity reciprocal effective mass tensor”),以叱及Μ*1分別代表電子及電洞,其定義: M—1 (E T) = e>Ef bz-—----- e,iJ F, Σ ifmKn),EF,T)d3k e>ef b.z. 為電子之定義,以及DETAILED DESCRIPTION OF THE INVENTION The present invention will be described in detail in the following description of the specification of the invention. However, the invention may be practiced in many different forms, and the scope of the invention is of course not limited to the embodiments shown in the drawings. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and the scope of the invention. Throughout the description of the present invention, the same drawing reference numerals are used to designate the same or equivalent elements, and the addition of 2rime) or multiple twisting symbols are used to indicate similarities in different embodiments. element. The present invention relates to controlling the properties of a semiconductor material at the level of atoms or molecules to achieve improved performance of the semiconductor device. Moreover, the present invention is also directed to enhancing the identification, creation, and use of materials for application to the conductive paths of semiconductor components. The theory presented by the Applicant of the present application shows that certain superlattice configurations disclosed herein can reduce the equivalent mass of the charge carriers and, by virtue of such reduction, can result in higher charge carrier mobility, but applications It is also stated that the scope of the invention is not limited to this theory. Among the documents in the art to which the present invention pertains, there are various definitions of equivalent masses for description. As a measure of the improvement in equivalent quality, the applicant uses "conductivity reciprocal effective mass tensor" to represent electrons and holes, respectively, and Μ*1. Definition: M-1 (ET) = e>Ef bz------- e,iJ F, Σ ifmKn), EF,T)d3k e>ef bz is the definition of electrons, and
MitAEF,T) Σ j (Vk^(k,n)),. (Vk£(k,n)).⑽k:),%^3k E<Ef B.Z. 0tj X l(l-nE(k,nXEF,T))d\ B.Z. 8 Ί308376 則為電洞之定義,其中f係為費米-狄拉克分佈 distribution),EF 為費米能量(Fermienergy),T 為溫度,E(k,n)為電子 在對應於波向量k及第η個能帶的狀態之中的能量,下標丨’及〗係對 應笛卡兒座標(Cartesian coordinates)x,y及ζ,積分係在布里羅因區 (B.Z.,Brill〇uinzone)進行’而加總則是在電子及電洞的能帶分別高於 及低於費米能量的能帶之中進行。 °MitAEF,T) Σ j (Vk^(k,n)),. (Vk£(k,n)).(10)k:),%^3k E<Ef BZ 0tj X l(l-nE(k,nXEF, T))d\ BZ 8 Ί308376 is the definition of the hole, where f is the Fermi-Dirac distribution, EF is Fermienergy, T is temperature, and E(k,n) is electron Corresponding to the energy in the state of the wave vector k and the nth band, the subscripts 及' and 〖 are corresponding to the Cartesian coordinates x, y and ζ, and the integral is in the Brillouin zone (BZ) Brill〇uinzone) is carried out in the band of electrons and holes with energies above and below Fermi energy. °
申請人對導電性反等效質量張量之定義,係使得材料之導電性反等效 質量張量之對應分量中的較大數值者,其導電性的張量分量(tens〇rial component)亦得以較大些。在此申請人再度提起下述理論,即此地所 描述說明之超晶格其針對導電性反等效質量張量所設定之數值,係可 增進材料的導電性質,諸如典型地可使電荷載體傳輸有較佳之方向。 適當張量項數的倒數,在此被稱為是導電性等效質量。換句話說,若 要描述半導體材料構造的特性,則前述電子/電洞的導電性等效質量, 以及在載體預定要傳輸的方向上的計算結果,便可用來分辨出A 已有增進的該些材料。 應用前述方式便可為特定目的而選出具有較佳能帶構造的材料。這樣 的一種實例可以是用於一半導體元件的通道區域之一超晶格25材 料。以下將先參考圖1所描述依據本發明之一包括超晶格25的平面 MOSFET20。其中描述依據本發明包括有超晶格25之一平面 MOSFET(planarMOSFET)20。然而,熟習本技藝者皆可理解,在此 所指材料係可應用於許多不同型態的半導體元件上,像是離散元件 (discrete devices)及/或積體電路等。 示的M〇SFET20包括一底材21,其具有位於其中之淺溝渠隔 離(shallow trench isolation,STI)區 80、8卜更特別地,MOSFET 元件 以是互補金氧半導體(CM〇S)元件,其包括\與?通道電晶體與 ^應的超晶格通道,熟悉此技藝者應可了解,其中STI區係用以電^ ,離鄰接的電晶體。舉例來說’底材21可歧-半導體(例如石夕) 氐材或一絕緣體上覆矽(silic〇n_〇n_insul s〇I)的底材 二Ϊ減,像^氧切,科祕他實施之二可 9 1308376 所示的MOSFET20更包括淡摻雜的源極/汲極延伸區22、23, 較濃摻雜的源極/汲極區26、27,以及介於其間由超晶格25所提供 的通道區。如圖所示,環狀植入物區(hai〇 ^ 被包括在介於源極與汲極區26、27之間,並位於超晶格25之下。源 極/汲極金屬石夕化物(8〇1!1^/(^118迅(^%6]〇層3〇、31覆蓋源極/、 汲極區,此為熟悉此技藝者所可了解者。如圖所示,閘極35包括一 閘極介電層37,其鄰接著由超晶格25所提供的一通道區,且閘電極 層36係位在閘極介電層之上。在圖示的M〇SFET2〇中還提供有側辟 隔絕層(sidewall spacer)4〇、4卜以及金屬石夕化物層34,其係^在閘g 極層36之上。Applicant's definition of the conductivity inverse equivalent mass tensor is the larger of the corresponding components of the conductivity inverse equivalent mass tensor of the material, and the tens〇rial component of the conductivity is also Can be bigger. The Applicant hereby reaffirms the theory that the superlattice described herein, which is set for the conductivity inverse equivalent mass tensor, enhances the conductive properties of the material, such as typically allows charge carrier transport. There is a better direction. The reciprocal of the appropriate number of tensor items is referred to herein as the conductivity equivalent mass. In other words, if the characteristics of the semiconductor material structure are to be described, the conductivity equivalent of the aforementioned electron/hole and the calculation result in the direction in which the carrier is intended to be transmitted can be used to distinguish that A has been improved. Some materials. Materials having a preferred energy band configuration can be selected for a particular purpose using the foregoing methods. An example of this may be a superlattice 25 material for one of the channel regions of a semiconductor component. A planar MOSFET 20 including a superlattice 25 in accordance with one of the present inventions will now be described with reference to FIG. There is depicted a planar MOSFET 20 comprising a superlattice 25 in accordance with the present invention. However, it will be understood by those skilled in the art that the materials referred herein can be applied to many different types of semiconductor components, such as discrete devices and/or integrated circuits. The illustrated M〇SFET 20 includes a substrate 21 having shallow trench isolation (STI) regions 80, 8 therein, and more particularly, a MOSFET device to be a complementary metal oxide semiconductor (CM〇S) device. It includes \ and? The channel transistor and the superlattice channel should be understood by those skilled in the art, wherein the STI region is used to electrically connect the adjacent transistor. For example, 'substrate 21 can be ambiguous-semiconductor (such as Shi Xi) coffin or an insulator on the substrate (silic〇n_〇n_insul s〇I), the substrate is reduced, like ^ oxygen cut, secret secretary The MOSFET 20 shown in the second embodiment of the invention may further include a lightly doped source/drain extension 22, 23, a more heavily doped source/drain region 26, 27, and a superlattice interposed therebetween. 25 channel areas provided. As shown, the annular implant region (here is included between the source and drain regions 26, 27 and below the superlattice 25. Source/dip metallization (8〇1!1^/(^118Xun(^%6)〇3〇, 31 covers the source/bungee area, which is familiar to those skilled in the art. As shown in the figure, the gate 35 includes a gate dielectric layer 37 adjacent to a channel region provided by superlattice 25, and gate electrode layer 36 is tied over the gate dielectric layer. In the illustrated M〇SFET2〇 A sidewall spacer 4, 4b, and a metal lithium layer 34 are also provided, which are above the gate g-layer 36.
要將超晶格的製程整合到現有技術的CM〇s流程中, 成於ST!區8〇 : 81之上的超晶格薄膜25移除,以防止了鄰^^牛= 之間發生短路或漏電的情形。更特別地參考圖2入至2D與圖3,製程 可由,材21開始,其具有形成於其中的STI區80、81,以及其上之 犧牲氧化層(sacrificial oxide layer)85與一 VT植入物84 (以一列“+,,號 代表)。以下面所將進一步描述的結晶矽超晶格來說,當犧牲氧化層 85被移除’而超晶格25被形成於底材21上時,矽沉積會造成 (也就是多晶體或非結晶的)石夕沉積物86、87覆蓋於STI區8〇、= 之上。然而如上所述,非單晶魏積物需要被移除 結構之間發生娜«電的情形。 «楼π件 儘管在某些實施射似相當直接的方法針對單—基線絲 area’AA)光阻遮罩88 (如圖2C所示)進行遮罩以 86、87 (如圖2D所示)的後續敍刻是可以接受的,但 下’這麼做會導致某些困難。更特別的,如果遮罩沒有^ STI邊緣上的非單晶石夕沉積物86 $一部份被光阻88所遮蔽》或者 在電漿姓刻過程中沒有充分的過侧(over_etch),那麼在ST 以及STI凹陷内的部份非單晶石夕沉積物可能會保持未被侧。因此 餘留為-鄰接主動元件的寄生元件,而鄰接STI區的 為通道阻絶鮮未群_係)會被不地蝴㈣下 ^ 摻雜物潛變(dopant creep)可能會非刻意地發生在鄰接非單晶‘夕 ,86 =不均勻的金屬碎化物與源極/汲極接面漏 — leakage)底材則可能會發生在鄰接間隙89之處。 1308376 因f 罩與叙刻操作可有利地予以修改,以便於STI區8。、81的 邊緣提供非單晶半導體_条或未_突起(誠^卿2、83 ϋ阻絕植人物,如圖1所示。再者,在STI區80、81上進行超 曰曰 的半導體單層的蠢晶成長過程中所產生的非單晶半導體沉 H开非單晶石夕。較佳地,非單晶街條82、83可有利地予以摻 ϊ做道阻雛人摻雜’如咖下騎透過數種製造範 =參考圖4至8 ’接下來將敘述用以製造半導體裝置之第一製程敕 ^程。從,方塊90的STI晶圓開始,在步驟方塊9卜Vt井被;To integrate the process of the superlattice into the prior art CM〇s process, the superlattice film 25 formed in the ST! area 8〇: 81 is removed to prevent a short circuit between the adjacent ^^= Or leakage. Referring more particularly to FIG. 2 to FIG. 2 and FIG. 3, the process can begin with material 21 having STI regions 80, 81 formed therein, and a sacrificial oxide layer 85 and a VT implant thereon. The object 84 (represented by a column "+,,"). In the case of the crystalline germanium superlattice, which will be further described below, when the sacrificial oxide layer 85 is removed, and the superlattice 25 is formed on the substrate 21 The strontium deposits cause (ie, polycrystalline or amorphous) stellate deposits 86, 87 to cover the STI region 8 〇, = above. However, as described above, the non-single crystal propagule needs to be removed from the structure. In the case of Na «Electricity. «The π piece is a fairly straightforward method for some single-baseline wire area'AA) photoresist mask 88 (shown in Figure 2C) to mask 86. Subsequent narration of 87 (as shown in Figure 2D) is acceptable, but the next 'doing so will cause some difficulties. More specifically, if the mask does not have a non-single-crystal deposit on the STI edge 86 $ Part of it is obscured by photoresist 88 or there is not enough over_etch in the process of plasma surname, then in S Some of the non-single-crystal deposits in the T and STI recesses may remain unsided. Therefore, the remaining is the parasitic element adjacent to the active device, and the adjacent STI region is the channel blocking the rare group. Do not bloom (4) lower ^ dopant creep (dopant creep) may occur unintentionally in adjacent non-single crystal 'eve, 86 = uneven metal fragmentation and source / drain junction leakage - leakage) The substrate may occur adjacent to the gap 89. 1308376 The f-cover and scribe operations can be advantageously modified to provide non-single-crystal semiconductor _ strips or un-protrusions at the edges of the STI regions 8. ^Qing 2, 83 绝 绝 绝 绝 绝 , , , , 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 。 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝 绝Preferably, the non-single-crystal street strips 82, 83 can be advantageously doped to prevent the doping of the cockroach, such as a coffee ride through several manufacturing models = reference to Figures 4 to 8 The first process for fabricating a semiconductor device will be described. Starting with the STI wafer at block 90, at step block 9 Vt Well
min的塾氧化物85,),隨後在步驟方塊92進行餘刻(i2〇A 二5 )。接著在步驟方塊93,暴露於氫氟酸(hydrofluoric acid,HF) 的HF異^°:1,5〇Α)。尤其是,塾氧化物85,的部份乾钱刻以及相當短 的HF暴蕗時間,舉例來說,可協助降低STI凹 ==,超晶格薄膜被沉積,其將進—步加以討二;^ 塊95則疋清洗步驟(spm/200:1,HF/RCA)。 Λ不,*上所述之單—基線Μ遮罩,在步驟方塊96, -過大Ν通道ΑΑ遮罩(如圖5Α與圖6Α所示),接著在步驟 材料,以及在步财塊98,_過A N财M 道阻絶植乂(如第九B圖所示)。在圖8A與8B,過大遮罩係 t考,1號版’與88P’標示,而N與P主動區㈣則分別以參 ί in與21p,標示。此外,反向N與P井係分取參考標號⑽ 興7印彳示不。 接著,在步驟方塊99,形成過大P通道aa遮罩(如圖5B所示 $著在步驟方塊100 ’以電漿蝕刻在鄰接p通道區的STI區之上的 單晶半導體材料,以及在步驟方塊UH,進行PFET通道阻入。 NFET與FET通道喊植人雛地係以—肖度或斜錢行,比如說% 度角,如圖6B所示,不過在此仍可使用其他的角度。如圖 通 道阻絕植人係關上的箭絲示。舉例麵,可胁nfet通 絶植入,而砷或磷可用於PFET通道阻絶植入。在stl區8〇,、81,的 凹陷(divot)内的桁條以及STI邊緣的未餘刻矽突起,係較佳地 11 1308376 阻絕植入物高度地反摻雜(counter-doped),以中和或減緩從源極一 $及 極區的摻雜物擴散進入STI凹陷之中的非單晶矽,或位於元件的通道 的角落之突起的擴散潛變(diffusion creep),以便有利地讓此寄生邊緣 元件具有較高的二極體崩潰電壓、較高的臨限電壓、以及較低的關閉 電流。針對P與N通道元件採用2種不同的過大的遮罩,可有利地在 非單晶矽蝕刻時保護AA對準標記,並且讓每一主動元件在其相反類 型元件進行if道阻絕植入時受到保護。Min 塾 oxide 85,), and then at step 92, the remainder (i2 〇 A 2 5). Next, at step 93, exposure to HF of hydrofluoric acid (HF) is 1,5 〇Α). In particular, some of the dry etching of bismuth oxide 85 and the relatively short HF violent time, for example, can help reduce the STI concave ==, superlattice film is deposited, which will be further discussed. ;^ Block 95 is the cleaning step (spm/200:1, HF/RCA). ΛNo, the single-baseline Μ mask described above, at step block 96, - oversized Ν channel ΑΑ mask (as shown in Figure 5Α and Figure 6Α), followed by the step material, and at step block 98, _Over the AN financial channel to block the plantation (as shown in Figure IX). In Figs. 8A and 8B, the oversized mask is t-marked, the 1st edition 'and 88P' are indicated, and the N and P active zones (4) are denoted by reference numerals and 21p, respectively. In addition, the reverse N and P wells are assigned reference numerals (10). Next, at step 99, an oversized P-channel aa mask is formed (as shown in FIG. 5B) at step block 100' to plasma etch the single crystal semiconductor material over the STI region adjacent the p-channel region, and in steps Block UH, PFET channel blocking. NFET and FET channel shouting people to the Shaw or oblique money line, such as the % degree angle, as shown in Figure 6B, but other angles can still be used here. As shown in the figure, the arrow is blocked by the implanted line. For example, the nfet can be implanted, and arsenic or phosphorus can be used for PFET channel blocking implantation. In the stl area, 8〇, 81, the recess (divot) The inner rafter and the unfinished ridges of the STI edge are preferably 11 1308376 to prevent the implant from being highly counter-doped to neutralize or slow down from the source to the $ and the polar regions. The diffusion of the dopant into the non-single crystal yttrium in the STI recess, or the diffusion creep of the protrusion at the corner of the channel of the element, in order to advantageously allow the parasitic edge element to have a higher diode breakdown voltage , higher threshold voltage, and lower shutdown current for P and N channels Member using two different masks too large, may be advantageously protected AA in the non-single-crystal silicon etch alignment marks, and so that each block the channel if the active elements are protected when implanted at the opposite type element.
一旦PFET通道阻絕植入完成後,在步驟方塊1〇2 (如圖8所示),進 行預先閘極清洗(SPM/HF/RCA) ’接著在步驟方塊1〇3,形成閘氧化物 37’(約20A),以及在步驟方塊1〇4 (如圖8B所示)’進行非單晶矽 閘,極36沉積與植入摻雜。在步驟方塊1〇5,進行閘極成像與触, 接著在步驟方塊106 ’形成側壁隔絕層40,、41,(例如ιοοΑ的氧化 物),以及在步驟方塊107 (如圖8C所示),進行淡摻雜(LDD)22,、 23 ’以及環狀42’、43’植入。然後在步驟方塊108 (例如19〇〇入的氧 化巧),針對側壁隔絕層40’' 41,進行餘刻。隔絕層4〇,、41,形成後, 接著在步驟方塊109進行源極/汲極26,、27,植入與回火(例如在 100(TC持續10秒),並且在步驟方塊110形成金屬矽化物,以提供圖 1所示的元件20〇更特別地,金屬矽化物可以是TiSi2 (例如沉積'欽 (Τι)、植入鍺、RTA@ 690。(:、選擇性剥除、接著RTA@ 75〇。〇。Once the PFET channel is blocked, complete the pre-gate cleaning (SPM/HF/RCA) in step 1〇2 (shown in Figure 8). Then in step 1〇3, gate oxide 37' is formed. (About 20A), and in step block 1〇4 (shown in Figure 8B) 'Perform a non-single crystal gate, pole 36 deposition and implant doping. At step block 〇5, gate imaging and touch are performed, then at step block 106', sidewall isolation layers 40, 41, (e.g., oxide of ιοοΑ) are formed, and at step block 107 (shown in Figure 8C), Light doping (LDD) 22, 23 ' and ring 42', 43' implantation are performed. Then, at step block 108 (e.g., 19 immersed oxidization), a residual is made for the sidewall isolation layer 40''41. The isolation layers 4, 41 are formed, followed by source/drain 26, 27, implant and temper at step 109 (eg, at 100 (TC lasts 10 seconds), and metal is formed at step block 110 Telluride to provide the element 20 shown in Figure 1 More specifically, the metal halide may be TiSi2 (e.g., deposited '钦, 锗, implant 锗, RTA@ 690. (:, selective stripping, followed by RTA) @75〇.〇.
圖12A與12B顯示元件結構在形成與閘極層36,平行和垂直的金屬 化物後之橫截面圖。在此些圖中,非單晶桁條82,、83, ^它們已經齡雜了通道_植人物。餘搞是 區内的矽凹處(recess)的深度,與用來移除在STI凹陷與STI邊緣内之 =晶街條與未侧突起82,、83,的過姓刻的量有關。另外,孰染此 技藝者應可了解,過多的凹處可能會導致增加的串 ^ 與LDD區之間失去接觸,此,根據所二的植:^源 廷些凹處的深度可能需要調整。 =的夕製二中,進行贿與聰的遮罩、蝕刻位於STI ^ 閘極氧化早87,、以及道阻絕植入等步驟,係於 包°在圖1所提出_代製程流程中,上述方 法係經修改,使得非單晶梦86,、87,的侧係於隔絕層姻步驟 1 12 1308376 驟方塊108,)後進行。另外,此-替代製程流程同樣也使用在間電極 層36”之上的氧化物或氮化物蓋層薄膜78”(如圖1〇B所示),以保 護閘極多晶矽(gatepolysilicon)在非單晶矽86”、87,,的蝕刻過程中不 會被姓刻。 在步驟方塊92’的乾钱刻結束後,在步驟方塊12〇,,進行清洗 (sPM/2〇〇:1,HF(5〇AyRCA),隨後進行邢預先清洗(職D,持續大 約1分鐘。就NFET與PFET遮罩沉積步驟(步驟方塊96,與99, 說’在此實例中是使用過大混合光阻遮罩(〇versizedhybridph〇t〇resist mask),如® l〇A所示。此外,在步驟方塊1〇4,的非單晶石夕閉電極層 沉積後,圖不之方法包括一 NSD遮罩步驟(步驟方塊⑵,),跟 在步驟方塊⑵’與m’的N+雜植人錢層氧化物_。其他與上 述方法不同的製程變異包括,在步驟方塊125,蝕刻STI區8〇”、^” 上之非單晶♦ 86”、87”(比如3GGA),接著在步驟方塊126,,餘 蓋層氧化物層(具有對矽的高選擇性)。剩下的製程流程盥圖4 討論的製程流程相似,故不再贅述^ 以下將參考圖13A與13B敘述另-可替代的製程流程。此一製程产 程採用一通用過大AA遮罩,用來姓刻STI區8〇”,、81,,,上之 ^ 石夕86”,、87,’’ ’接著是2個獨立的遮罩步驟,用以讓突起開 曰曰 opening)成像。更特別地’係使用npet通道阻絕遮罩13〇n”盘押 ,阻《罩13Gp,,。NFET與PFET遮罩步驟後進行通道阻絕植入 ^驟便掺雜在突起開口中的非單㈣。前述的步驟可於間極氧化 步驟之前進行。 ^可了解的是,以上概述之示範的製程流程可有利地在成長閘極 物之刖,先蝕刻STI區上的非單晶半導體材料。此外,以適當能 摻雜劑量植人之通道阻職人物,可電性中和來自鄰接的源極^ 之摻雜物’避倾散至贿未侧賴·娜,其t超晶格 不適恰地隱藏在STI氧化物上的非單晶料主動區邊緣或突起之凹、入、 的STI凹陷内,因為過大的主動區遮罩而包圍主動區。當然,應 ,的是’在抑的實施方式中,除了上述範例的材料和製程流^ 卜’也可採用其他合適的材料以及製程參數。 以下將討論用於MOSFET20的通道區之改良材料或結構,其中 13 1308376 MOSPEJ,#有的能帶結構,使得電子以及/或者電洞的適當導電性 有效質量係實質地小於矽的對應數值。額外地參考圖14與圖15,超 晶格25具有一構造,係於原子或分子層級控制,並可利用已知的原 子或分子層沉積的技術製作形成。超晶格25包括有以堆疊形式安排 的複數個層群組(layer groups) 45a-45n,如上所述,透過參考由圖14 示意之橫截面圖也許可最為清楚地瞭解。 =曰^5 ^軸層群組45a_45n,如断林含有分別界賴應基底 f ‘體^伤(base semiconductorportion)46a-46n 的複數個堆疊的基底 半導體單層(basesemiconductormonolayer)46,以及其上的一能帶修改 層(energy-bandmodifyinglayer) 50。為了說明清楚之故,能帶修改層Figures 12A and 12B show cross-sectional views of the element structure after forming a metallization parallel and perpendicular to the gate layer 36. In these figures, non-single-crystal rafters 82, 83, ^ have been mixed with channels. The remainder is the depth of the recess in the zone, which is related to the amount of the surname used to remove the = and 83 sides of the STI recess and the STI edge. In addition, those skilled in the art should be aware that excessive recesses may result in loss of contact between the increased string ^ and the LDD region, which may need to be adjusted depending on the depth of the implant. = In the eve of the second system, the bribe and Cong mask, the etching is located in the STI ^ gate oxidation early 87, and the step of the barrier to implant, etc., in the package ° in the proposed generation process, the above The method was modified such that the side of the non-single crystal dreams 86, 87 was followed by the isolation layer step 1 12 1308376, block 108,). In addition, this alternative process also uses an oxide or nitride cap film 78" over the inter-electrode layer 36" (as shown in Figure IB) to protect the gate polysilicon in the non-single The wafers 86", 87, are not engraved by the surname during the etching process. After the completion of the step 92', the cleaning is performed (sPM/2〇〇:1, HF (in the step block 12〇). 5〇AyRCA), followed by Xing pre-cleaning (O'D for about 1 minute. The NFET and PFET mask deposition steps (steps 96, and 99, saying 'in this example is using an oversized mixed photoresist mask ( 〇versizedhybridph〇t〇resist mask), as shown by ® l〇A. In addition, after the deposition of the non-single-crystal slab electrode layer in step block 〇4, the method of the figure includes an NSD masking step (step Block (2),), followed by step (2) 'and m' of N+ hybrid money layer oxide _. Other process variations different from the above method include, at step block 125, etching the STI region 8 〇", ^" Non-single crystal ♦ 86”, 87” (such as 3GGA), then in step 126, the cover layer The chemical layer (having high selectivity to germanium). The remaining process flow is similar to the process flow discussed in Figure 4, so it will not be described again. The following will describe another alternative process flow with reference to Figures 13A and 13B. The production process uses a universal oversized AA mask, which is used to name the STI area 8〇", 81,,, on the ^ stone eve 86", 87, '' ' followed by 2 independent mask steps for Let the protrusions open and image. More specifically, 'use the npet channel to block the mask 13〇n' to discard, block the cover 13Gp,, and the NFET and PFET mask steps are followed by channel blocking implants. Non-single (four) mixed in the opening of the protrusion. The foregoing steps can be performed before the inter-polar oxidation step. ^ It is understood that the exemplary process flow outlined above can advantageously etch the STI region after growing the gate On the non-single-crystal semiconductor material. In addition, the person with a suitable doping dose implanted in the channel, can electrically neutralize the dopant from the adjacent source ^ to avoid dumping to the bribe a non-single crystal material master whose t superlattice is not properly hidden on the STI oxide In the STI recess of the edge or protrusion of the moving area, the active area is surrounded by the excessive active area mask. Of course, it should be, in the embodiment of the embodiment, except for the material and process flow of the above example ^ Other suitable materials and process parameters can also be used. The improved material or structure for the channel region of MOSFET 20 will be discussed below, where 13 1308376 MOSPEJ, # has a band structure that allows proper conduction of electrons and/or holes. The effective mass is substantially less than the corresponding value of 矽. With additional reference to Figures 14 and 15, superlattice 25 has a configuration that is controlled at the atomic or molecular level and can utilize known atomic or molecular layer deposition techniques. Production formation. The superlattice 25 includes a plurality of layer groups 45a-45n arranged in a stacked form, as described above, perhaps best understood by reference to the cross-sectional views illustrated by Figure 14. =曰^5^Axis layer group 45a_45n, such as a broken forest containing a plurality of stacked base semiconductor semiconductor layers 46a-46n, and a plurality of stacked base semiconductor monolayers 46, and thereon An energy-band modifying layer 50. For clarity, it can be modified
50於圖14之中係以雜點加以標示。 乂 圖中„廿帶修改層50包含有一非半導體單層(職-semiconductor ^ ^制在與其鄰接之基底半導體部份的晶體晶格内。 ΐ 方ΐίί ^ 祝·4511中相對置的基底半導體單層46 起。舉例來說,树質單層46的情況之中, 群組的較上端或頂端半導體單層中的某轉原子,會與群 45a-45n 中相二二f思, (c〇vaJ^ 導體原子(亦即本例中的氧^故層中的某些石夕原子會被結合至非半 在其他實施例之中,多於一個非丰導舻 能帶修改層5G中的非半導體單層的數量,$佳=行的。例如’ 層,以藉此提供所欲獲得_帶修改層特性、較佳者可小於約5個單 整體區塊之形式成係代表,如果依 體。也就是,如熟悉此技藝者所可理解,諸=半導體或半導 t並不必鋪現鮮絲絲魏 1308376 申請人仍聲明本發明之範4不應限定於其理論上,亦即能帶修改声5〇 及其所鄰接之基底半導體部份46a-46n ’會使超晶格25在平行於> 面之=向上的電荷載體,較之無此安排者,具有較低的適當導生^ 效質量。以另-種方式考慮,此平行方向係與堆疊的方向正交 修改層50亦可能使超晶格25具有共同能帶((χ)η_η_^ ^ 揮其作為賴或超晶格《上或下方區域之間 的心缘„„之作用。再者,如上所指’此構造亦可有利地發揮 社顧餘超晶格25之上層财賴的摻雜質 以及/或者材料的溢散或者擴散,以及載體流動。 、 t發,之理論齡,該超晶格25基於較低之導祕等效質量 ,、、、此t排者,該超晶格25提供一較高的電荷載體移動性。, $述超晶格25之特性,並非在每種用途中都須應用。例如、,、如‘ S本項技術者所可萌,在某些顧巾,超晶格25可僅 ^ UJ/絕緣之特性或其動性加強,或者在其他應财,則可利用“ 一巧㈣1_52係位於超晶格25的上端層群組45 基底半導體單層46。蓋層52可以擁有2至⑽ίίί =底+導體,且其較佳者應為1G至5G個單層。其他的厚度也可^ ,-基底半導體部份46a — 46n,可以包含由 導體,以及·解_驗成料蚊巾 體。當然了,如熟悉此技藝者所可理解的,IV ^缺 族辭導體。尤妓,基辭《可 ίΐίίΞ^非可i包體t有由諸如氧,氮’氟’以及碳_氧等的組合 鄰層進行沉積_餘驗行,《得目 或r合r可為符合特定半導體的製作心 15 1308376 應予注意的是,單層(mon〇layer)一詞在此亦應包括單原子層㈤ngie =11Clayer)以及單分子層(singlem〇lecularlayer)。另亦應注意的是, .,早原子層所提供的能帶修改層5〇,亦應包含其層中並未完全填 ^可能原子位置的單層。例如,參考圖ls,其中顯* 了一種4/1、的 ,構造’其係以梦作為基底半導體材料及以氧作為能帶修改材料。龙 中只有半數的氧的可能位置被佔滿。 ” 施例之中以及/或者在不同材料的情況之下,如同熟悉此 ’較佳細係從約人分之_至半數的氧的可能位置被佔 滿,,、、、、而其他的範圍亦可被用在特定的實施例中。 =於矽及氧目前储廣泛地躺於-㈣轉 ^匕得以立即地使財發日月所描述的這m者 爾術。耻,刪於本1=^解 的+導體70件即得以立即地利用並實施本發明所揭示之超晶格25鮮 之ί藝者所可以理解的情形,在本示意圖中亦可看出,i —特原子並未沿一平面精確地排列。舉例而 明本發明之射不舰定於其理論上,就—超晶格而+, 向上電子及電_紐鶴性。例如, 電子 果,ί體區塊的_算_值為^的^^ 超日日格則為0.16,兩者比例為〇 44。 bl/〇 = 特性對某些半導體元件而言可能有利,在1 他+導體兀件之中,平行於層群組的群組平 加動性,則可能更為有利。對熟悉此技藝者而t,增 洞的動性,或只有增加其中一種電荷_‘2:^^電 在超晶格25之4/1Si/0實施例中,其較低導電性等效質量可能要比 16 1308376 is;=2f=,且此情形就 在其他實_巾,雛的作法為爾超在元件巾的 格25的-或更多個層群組45為實質地未摻雜__)。置超曰曰50 is indicated by a dotted line in FIG. In the figure, the 修改 tape modification layer 50 includes a non-semiconductor monolayer (the-semiconductor is formed in the crystal lattice of the base semiconductor portion adjacent thereto. ΐ方ΐίί ^ 祝 4511 opposed to the base semiconductor single For example, in the case of the tree single layer 46, a certain atom in the upper end or the top semiconductor monolayer of the group will be associated with the group 45a-45n, (c〇 vaJ^ conductor atoms (that is, some of the oxygen atoms in this example will be bound to non-half in other embodiments, more than one non-conducting band can modify the non-layer 5G The number of semiconductor single layers, $good = row. For example, 'layer, in order to provide the desired layer with modified layer characteristics, preferably less than about 5 monolithic blocks, if the body is That is, as will be understood by those skilled in the art, the semiconductors or semi-conductors t do not have to be laid out. 1 Applicant still claims that the invention 4 should not be limited to its theory, that is, the band Modifying the acoustic 5 〇 and its adjacent base semiconductor portion 46a-46n 'will cause the superlattice 25 to be flat The charge carrier of the > face = upward has a lower proper quality of conductance than the one without the arrangement. In another way, the parallel direction is orthogonal to the direction of the stack. It is possible that the superlattice 25 has a common energy band ((χ)η_η_^^" acts as a "heart" between the upper or lower regions of the Lai or superlattice. Again, as indicated above, this structure is also It can be beneficial to play the doping of the upper layer of the super-lattice 25 and/or the scattering or diffusion of the material, and the carrier flow. The theoretical age of the t-cell, the superlattice 25 is based on the lower The super-lattice 25 provides a higher charge carrier mobility. The characteristics of the superlattice 25 are not applicable in every application. For example, ,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, (d) 1_52 is located in the upper end layer group 45 of the superlattice 25, the base semiconductor single layer 46. The cap layer 52 can have 2 to (10) ίίί = bottom + Conductors, and preferably should be 1G to 5G single layers. Other thicknesses can also be used, and the base semiconductor portions 46a-46n can contain conductors, and solutions to the mosquito body. Of course As can be understood by those skilled in the art, IV ^ lacks the family conductor. Youyi, the basic word "可 ΐ Ξ Ξ 非 非 包 包 包 有 有 有 有 有 包 包 包 包 包 包 包 包 包 包 组合 组合 组合 组合 组合 组合 组合 组合 组合 组合 组合 组合 组合 组合The layer is deposited _ residual inspection, "destination or r-r can be made to meet the specific semiconductor fabrication core 15 1308376 It should be noted that the word mono layer (mon〇layer) should also include the monoatomic layer (5) ngie = 11Clayer) and a single molecule layer (singlem〇lecular layer). It should also be noted that the band modification layer 5 provided by the early atomic layer should also include a single layer in the layer that is not completely filled with possible atomic positions. For example, reference is made to Figure ls, in which a 4/1, "structure" is used as a base semiconductor material and oxygen as an energy band modification material. Only half of the oxygen's possible locations in the dragon are filled. In the case of the application and/or in the case of different materials, as is familiar with this, the preferred position is from the occupant to the half of the possible position of oxygen is occupied,,,,, and other ranges It can also be used in a specific embodiment. = The current storage of sputum and oxygen is widely lying in - (4) 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕 匕The +conductor 70 piece of the conductor can be immediately utilized and implemented by the present invention. The superlattice 25 can be understood by the art. It can also be seen in the schematic diagram that i-specific atoms are not Exactly arranged along a plane. For example, the invention of the invention is based on its theory, namely - superlattice and +, upward electrons and electricity_new crane. For example, electronic fruit, _ body block _ The ^^ super-day grid with a value of ^ is 0.16, and the ratio of the two is 〇44. The bl/〇= characteristic may be advantageous for some semiconductor components, in the 1+conductor element, parallel to It may be more advantageous to group the groups of the layer groups. For those who are familiar with the art, the mobility of the holes is increased, or only increased. The charge _'2: ^^ electricity in the 4/1Si/0 embodiment of the superlattice 25, its lower conductivity equivalent mass may be more than 16 1308376 is; = 2f =, and this situation is in other real _ towel, the practice of the younger is in the cell 25 of the component towel - or more of the layer group 45 is substantially undoped __).
額外地同時參考圖16,接著將依據本發明描述具有不同性質的 25,的另二實施例。在此實施例之中顯示出3/1/5/1之重覆模:日曰二 別的是’最底下的基底半導體部份伽,具有3個單層,而第、靥 的基底半導體部份46b’則有5個單層。此種組合模式在整個超曰格 25’之中重覆。每-能帶修改層5〇,則各包括一單一的單層。就t Si/O的此種超晶格Μ,而言,其電荷載體動性的增進是與各 中的指向無關的。圖16之巾在此未制提及的其他構造部份係 述圖14中所討論者類似’故在此不再重覆討論。 ”/、 在某些元件實補0,超晶格25的财基辭轉雜4&46η, 其厚度可能為相同數目單層疊合的厚度。在其他的實施例, 某些基底半導體翁46a_46n,其厚度可能是林隨目單層疊合之 厚度。在另外的實施例之中,所有基底半導體部#46a_46n 則可能是不同數目單層疊合之厚度。 〃 圖17A至圖17C顯示應用密度功能理論pensity Functi〇nal ^ DFT)所計算的能帶構造。本技藝帽廣為f知的是,DFT通常低;古 能帶間隙的絕對值。因此間隙以上的所有能帶皆可利用適當的「剪刀 形修(“seises correction”)加以偏移。不過,此一能帶的形狀則是 公δ忍运較為可罪。垂直的能量軸(verticai energy axes)應在此等認知之 下加以考量。 圖17A為整體區塊的矽(bulk silicon,以實線表示)以及圖丨4中所顯 示之4/1 Si/O超晶格25 (虛線表示),兩者由迦碼點⑹處計算而得之 能帶構造之曲線圖。雖然圖中其(〇〇1)之方向確與沿之一般單位晶元 的(001)方向相符,然其方向係指4/1 Si/O結構之單位晶元(unitcell)而 非Si的一般單位晶元’並因而顯示了 Si傳導能帶最小值的期待位置。 圖中的(100)及(010)方向係與Si之一般單位晶元的(110)及(_11〇)方向 符合。熟悉此技藝者可以理解,圖中Si之能帶係以摺合顯示,以表 17 1308376 示它們在4/1 Si/O構造之適當的反晶格方向(recipr〇cal lattice directions)。 财可看出,與整寵塊哪i)她之下,4/1 Si/〇構造 ^係位騎碼點(G)之處’而魏絲帶的最小侧是域在_) ^向上:在布里羅因區㈣丨⑽丨請㈣的邊緣^之為⑶之處。! 亦可以注意到,4/1 Si/Ο構造與Si的料能帶最小值之曲率,里相較 有較大的曲率,這是因為額外氧層引人了擾亂所造i的能 圖為整體區塊石夕(實線)以及圖w之4/1,超晶格μ (虛線), =由Z點之處計算得的能帶構造之曲線圖。此圖中所顯示的是( 方向上鍵結能帶之增加曲率。 圖17f為整體區塊石夕(實線)以及圖16中所顯示之5/1/3/isi/〇超晶格 ’兩者由迦碼及z點之處計算得之能帶構造之曲線圖。由於 3構造的對稱性,在_及_)方向上計算所得的能帶結 的。因此,在平行於各層的平鸯,亦即,在垂直於卿)的堆 豐方向上’導電性等效質量及動性可以預期是等向性的。注意到在 5/lf/l Si/O的實例之巾’料歸最小值及鍵結能帶最大值兩者皆位 於或近於Z點之處。 雖^曲巧增加是等效質量減小的—指標,但經由導電性反等效質量 張量的計仍可以進行適當齡較及判別。此使縣案申請人進一 ==5/1/3/1的超晶格25’實質上應是直接的能帶間隙。如同熟悉 此技藝者所可謂_,可絲轉飾ptiealtransitiGn㈣適當矩陣 早7L(matnX element)乃是區別直接與間接能帶間隙行為的另一種指 標0 ,於本技藝者在瞭解了本案於前述說明文字及附圖所描述的發明揭 不内容崎況之下,當可推知瞭麟對本發明的許多修改變動以及i 他不同的實施例作*。因此,應予瞭解献,本發明之範脅不應限& ^刖述^實施例的範圍’其他的修改變動及其他實施例仍 發明之精神範疇。 18 1308376 【圖式簡單說明】 依據本發明—糊元件之_截_,其中包 的潛在困難。之域面圖顯不圖1的半導體元件之形成以及與其相關 =顯不圖1半導體讀的—部份在經過閘電極成像與钱刻後之上視 ® ^為盥;m應圖1的半導體元件之製程流程。 視圖,應用於圖4方法之刪丁與聰通道阻絕遮罩之上 圖7為經過成4與严阻缉植入步驟之橫截面圖。 圈’其,㈣通 Ϊ0 以及閘極沉積/植人等步驟導熱刻 '通道阻絕植入' ί 1=^2=-9=二隔騎形齡·該元件賴之上視圖》 與間極層平行和垂直旬金屬石夕化物後該元 圖13A與13B為根據製作圖1半導體元件 ±φ,γ3· ¢1¾ 突起通道阻絕遮罩步驟之^觸牛導·件之另-種製程的主動區與 1曰曰格Υ應另一實施例之大比例放大橫截面圖,該 ϋ7Βϋί〇技藝中之整體區塊石夕以及圖14中所顯示之4/1 si/0超 U為^技藝中之整體區塊石夕以及圖16中所顯示之5/1/3/lSi/O 超曰曰格,兩者由迦碼及Z狀處計算狀能轉^曲線圖。 【主要元件符號說明】 19 1308376Referring additionally to Figure 16, at the same time, another embodiment of 25 having different properties will be described in accordance with the present invention. In this embodiment, a 3/1/5/1 overmolding mode is shown: the second is the 'bottom-base semiconductor portion gamma, which has three single layers, and the first and second base semiconductor portions. Part 46b' has 5 single layers. This combination pattern is repeated throughout the Super 25 25'. Each layer can be modified to include a single single layer. In the case of such superlattice t of t Si / O, the enhancement of the charge carrier kinetics is independent of the orientation in each. The other structural portions of the towel of Fig. 16 which are not mentioned herein are similar to those discussed in Fig. 14 and will not be discussed again. "/, in some components, the complement of 0, the superlattice 25 of the financial base 4 & 46n, the thickness may be the same number of single-stacked thickness. In other embodiments, some of the base semiconductors 46a_46n, The thickness may be the thickness of the lining of the forest. In other embodiments, all of the base semiconductor portions #46a-46n may be different thicknesses of a single stack. 〃 Figures 17A to 17C show the application of density function theory pensity Functi〇nal ^ DFT) The calculated energy band structure. The skill cap is widely known that the DFT is usually low; the ancient energy has an absolute value of the gap. Therefore, all the energy bands above the gap can be properly scissor-shaped. The repair ("seises correction") is offset. However, the shape of this energy band is more sinful than the δ. The vertical energy axis (verticai energy axes) should be considered under such cognition. Figure 17A It is the bulk silicon (indicated by the solid line) and the 4/1 Si/O superlattice 25 (indicated by the dotted line) shown in Fig. 4, which are calculated by the code point (6). Can be a structure of the curve. Although it is in the figure ( The direction of 〇1) does correspond to the (001) direction along the general unit cell, but the direction refers to the unit cell of the 4/1 Si/O structure rather than the general unit cell of Si and thus The expected position of the Si conduction band minimum is shown. The (100) and (010) directions in the figure correspond to the (110) and (_11〇) directions of the general unit cell of Si. It will be understood by those skilled in the art that In the figure, the energy bands of Si are shown in folds, and they are shown in Table 17 1308376 for the appropriate anti-grid direction of the 4/1 Si/O structure. It can be seen that the whole pet block i) Under her, 4/1 Si/〇 structure ^ is the location of the code point (G) 'and the smallest side of the Wei ribbon is the domain _) ^ Up: in the Briorin area (four) 丨 (10) 丨The edge of (4) is (3). It can also be noted that the curvature of the 4/1 Si/Ο structure and the material band of Si has a larger curvature, because the extra oxygen layer is introduced. The energy map made by human disturbance is the whole block Shi Xi (solid line) and the figure w/4/1, superlattice μ (dashed line), = the curve of the energy band structure calculated from the Z point Shown in this figure It is (the direction of the bond energy band increases the curvature. Figure 17f is the overall block Shi Xi (solid line) and the 5/1/3/isi/〇 superlattice shown in Figure 16] And the curve of the energy band structure calculated at the z-point. Due to the symmetry of the 3 structure, the obtained energy band is calculated in the _ and _) directions. Therefore, in the plane parallel to the layers, that is, Conductive equivalent mass and kinetics can be expected to be isotropic in the direction of the stacking perpendicular to the). It is noted that in the example of 5/lf/l Si/O, the material minimum and the maximum bond energy band are both at or near the Z point. Although the increase in the curvature is an index of the equivalent mass reduction, the appropriate age comparison and discrimination can still be performed by the conductivity inverse equivalent mass tensor. This allows the county applicant to enter a ==5/1/3/1 superlattice 25' which should be essentially a direct energy gap. As is familiar to the skilled person, _, can be transferred to ptiealtransitiGn (four) appropriate matrix early 7L (matnX element) is another indicator to distinguish between direct and indirect band gap behavior 0, the artist knows the case in the above description And the invention described in the accompanying drawings, it is to be understood that many modifications of the invention and the various embodiments of the invention can be deduced. Therefore, it is to be understood that the scope of the invention is not limited to the scope of the embodiments of the invention, and other modifications and other embodiments are still within the spirit of the invention. 18 1308376 [Simple Description of the Drawings] According to the present invention, the blunt element of the paste element has a potential difficulty in the package. The domain diagram shows the formation of the semiconductor component of FIG. 1 and its correlation = the semiconductor read of FIG. 1 is partially reflected by the gate electrode and the memory of the gate; Process flow of components. The view, applied to the method of Figure 4, is a cross-sectional view of the implanted step and the sturdy barrier. Circle 'its, (4) through Ϊ 0 and gate deposition / implanting steps, etc., heat conduction engraved 'channel blocking implant' ί 1=^2=-9=two-sitting age · the element depends on the top view and the interlayer After the parallel and vertical metallization, the elements 13A and 13B are the active regions of another process according to the fabrication of the semiconductor device of FIG. 1 by the ±φ, γ3·¢13⁄4 protrusion channel blocking step. And a larger scale enlargement cross-sectional view of another embodiment, the overall block of the ϋ7Βϋί〇 technique and the 4/1 si/0 super U shown in FIG. 14 are in the skill The overall block Shi Xi and the 5/1/3/lSi/O super cell shown in Figure 16 are calculated from the Gamma and Z-shapes. [Main component symbol description] 19 1308376
20 MOSFET 21、21’底材 21η’ Ν主動區 21ρ’ Ρ主動區.,20 MOSFET 21, 21' substrate 21η' Ν active region 21ρ' Ρ active region.,
22 源極區 22, LDD 23 淡極區 25 超晶格 26、 26’ 源極區 27、 27’ >及極區 30 源極金屬矽化物層 31 汲極金屬矽化物層 32 源極接點22 source region 22, LDD 23 pale region 25 superlattice 26, 26' source region 27, 27' > and polar region 30 source metal germanide layer 31 germanium metal telluride layer 32 source contact
33 汲極接點 34 金屬石夕化物層 35 閘極 36、 36’、36”閘電極層 37、 37’ 閘氧化物 38 閘電極層 40、 40’ 側壁隔絕層 41、 41’ 側壁隔絕層 42、 42’ 環狀植入物區 43、 43’ 環狀植入物區 45a~45n、45a'~45n'堆叠層組 46 基底半導體單層33 bungee contact 34 metallization layer 35 gate 36, 36', 36" gate electrode layer 37, 37' gate oxide 38 gate electrode layer 40, 40' sidewall isolation layer 41, 41' sidewall isolation layer 42 , 42' annular implant region 43, 43' annular implant region 45a~45n, 45a'~45n' stacked layer group 46 base semiconductor monolayer
46a〜46n、46a'〜46η’ 基底半導體部份 50'50' 能帶修改層 52、52'蓋層 78” 氧化物或氮化物蓋層薄膜 79η, 反向Ν井 79ρ’ 反向Ρ井 80、 80’、80”STI 區 81、 81’、81”STI 區 82、 82’非單晶桁條 83、 83’非單晶桁條 84 VT植入物 85 犧牲氧化層 85, 墊氧化物 86、86’、86”非單晶矽沈積物 20 130837646a~46n, 46a'~46n' base semiconductor portion 50'50' can be modified with layer 52, 52' cap layer 78" oxide or nitride cap film 79n, reverse well 79ρ' reverse well 80 , 80', 80" STI area 81, 81', 81" STI area 82, 82' non-single crystal strip 83, 83' non-single crystal strip 84 VT implant 85 sacrificial oxide layer 85, pad oxide 86 , 86', 86" non-single crystal germanium deposits 20 1308376
87、87’、87”非單晶石夕沈積物 88 光阻 88η’ 過大Ν遮罩 88ρ’ 過大Ρ遮罩 89 間隙 130n” NFET通道阻絕遮罩 130p” PFET通道阻絕遮罩 圖4的流程 90 STI晶圓 91植入VT井(透過150Α的墊氧化物85,) 92進行乾蝕刻(120A的氧化物) 93 暴露至氫氟酸(hydrofluoric acid,HF)中(SCl/100:l,5〇A) 94沉積超晶格薄膜(5〇A) 95 清洗步驟(SPM/200:1,HF/RCA) 96形成過大的N通道AA遮罩 97以電漿蝕刻STI區之上的超晶格薄膜 -98 NFET通道阻絶植入 99過大的P通道AA遮罩 100以電漿蝕刻STI區之上的超晶格薄膜 101 PFET通道阻絶植入 102進行預先閘極清洗(SPM/HF/RCA) 103形成閘氧化物(約20A) 104非單晶矽閘電極沉積與植入摻雜 105閘極成像與蝕刻 106形成側壁隔絕層(100A) 107 LDD與環狀植入物 108形成側壁隔絕層(1900人) 109源極/没極植入與回火(在i〇〇〇〇c持續丨〇秒) 110形成金屬矽化物(沉積鈦(Ti)、植入鍺、RTA @ 690«>c、選擇性杀丨 除、接著RTA@750°C) 〇 、伴旺利 圖9的流程 90’STI晶圓 91植入VT井(透過150A的墊氧化物85,) 92進行乾钱刻(120A的氧化物) 12〇 進行清洗步驟(SPM/200:1,HF (5〇AyR_CA) 121’HF預先清洗(100:1),持續大約i分鐘 2187, 87', 87" non-single crystal slab deposit 88 photoresist 88 η 'over large Ν mask 88 ρ ' over large Ρ mask 89 gap 130 n ” NFET channel blocking mask 130 p ” PFET channel blocking mask flow of Figure 4 STI wafer 91 is implanted into VT well (through 150 Α pad oxide 85) 92 dry etched (120A oxide) 93 exposed to hydrofluoric acid (HF) (SCl/100: 1,5〇 A) 94 deposited superlattice film (5〇A) 95 Cleaning step (SPM/200:1, HF/RCA) 96 forms an oversized N-channel AA mask 97 to plasma etch the superlattice film over the STI region -98 NFET Channel Blocking 99 Oversized P-Channel AA Mask 100 to Plasma Etch Super-lattice Film on STI Area 101 PFET Channel Blocking Implant 102 for Pre-Gate Cleaning (SPM/HF/RCA) 103 forming a gate oxide (about 20A) 104 non-single crystal gate electrode deposition and implantation doping 105 gate imaging and etching 106 forming a sidewall isolation layer (100A) 107 LDD and annular implant 108 form a sidewall isolation layer ( 1900 people) 109 source / immersion implantation and tempering (last 丨〇 seconds in i〇〇〇〇c) 110 formation of metal telluride (deposited titanium (Ti), implanted 锗, RTA @ 690«>c, selective killing, followed by RTA@750°C) 〇, with the flow of Figure 9 'STI wafer 91 implanted in VT well (through 150A pad oxide 85,) 92 for dry money engraving (120A oxide) 12〇 for cleaning step (SPM/200:1, HF (5〇AyR_CA) 121'HF pre-cleaning (100:1) for about i minutes 21
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| US9941359B2 (en) | 2015-05-15 | 2018-04-10 | Atomera Incorporated | Semiconductor devices with superlattice and punch-through stop (PTS) layers at different depths and related methods |
| EP3669401B1 (en) * | 2017-08-18 | 2023-08-02 | Atomera Incorporated | Manufacturing method for a semiconductor device including the removal of non-monocrystalline stringer adjacent a superlattice-sti interface |
| CN115360232B (en) * | 2022-08-24 | 2025-09-05 | 南京信息工程大学 | Pocket-structured Si/Ge heterojunction gate-all-around tunneling field-effect transistor and preparation method thereof |
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| JP2009529780A (en) | 2009-08-20 |
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