TWI470796B - Power ldmos transistor - Google Patents
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Description
本發明係關於半導體結構且更加明確地關於橫向擴散MOS電晶體(LDMOS)與製造其之方法。The present invention relates to semiconductor structures and more specifically to laterally diffused MOS transistors (LDMOS) and methods of fabricating the same.
功率MOSFET(金屬氧化物半導體(MOS)場效電晶體(FET))係(例如)用作為電切換器,以供高頻PWM(脈衝寬度調變)應用,例如電壓調節器及/或功率應用中之負載切換器。當用作為負載切換器,其中切換時間通常係十分長時,該等切換器之成本、大小與導通電阻係主要設計考量。當用於PWM應用時,該等電晶體必須在切換期間展現小功率損失,其會附帶一額外的需求,即小內部電容,因而會使MOSFET設計富挑戰性且往往較昂貴。已對閘極至汲極(Cgd)電容投注特別的注意力,乃因此電容會決定在切換期間電壓瞬變時間,且係影響該切換功率損失最重要的參數。Power MOSFETs (MOSFETs) are used, for example, as electrical switches for high frequency PWM (Pulse Width Modulation) applications such as voltage regulators and/or power applications. Load switcher in the middle. When used as a load switch, where the switching time is usually very long, the cost, size and on-resistance of the switches are primarily designed. When used in PWM applications, the transistors must exhibit low power losses during switching, which is accompanied by an additional requirement, namely small internal capacitance, which makes the MOSFET design challenging and often expensive. Special attention has been placed on gate-to-drain (Cgd) capacitors, so the capacitance determines the voltage transient time during switching and is the most important parameter affecting the switching power loss.
關於先前技術橫向擴散功率MOSFET裝置之範例係由D'Anna等人之美國專利第5,949,104號與D'Anna等人之美國專利第6,831,332號提供,其全部係以提及之方式併入本文中。兩裝置皆採用厚的磊晶層,以達目標RF應用所需之高崩潰電壓(>60 V)。欲使該裝配件中之寄生源極電感降至最低,兩裝置係皆設計於P+基板上,並導致源極電極出現在晶粒之背側。該厚磊晶層與P+基板會使該裝置產生一高導通電阻(Rds ,on ),其係無法為功率管理應用所接受。An example of a prior art laterally-dividing power MOSFET device is provided by U.S. Patent No. 5,949,104 to D'Anna et al., and U.S. Patent No. 6,831,332 to D. Both devices use a thick epitaxial layer to achieve the high breakdown voltage (>60 V) required for target RF applications. To minimize parasitic source inductance in the assembly, both devices are designed on the P+ substrate and cause the source electrode to appear on the back side of the die. The thick epitaxial layer and the P+ substrate cause the device to generate a high on-resistance (R ds , on ) that is not acceptable for power management applications.
另一先前技術橫向擴散金屬氧化物半導體裝置係揭示於Rumennik之美國專利第6,600,182號中,其標題為"High Current Field-Effect Transistor"。該Rumennik裝置包括一汲極區域,其具有一穿透該磊晶層而垂直延伸以連接至該基板的第一部分與一沿該裝置之頂表面而橫向延伸的第二部分。該裝置具有低特定導通電阻並支持高電流流動。然而,該裝置之崩潰電壓係高度取決於該汲極區域之第一部分的位置,其會使該裝置之製造容限窄化。Another prior art laterally diffused metal oxide semiconductor device is disclosed in U.S. Patent No. 6,600,182 to Rumennik, entitled "High Current Field-Effect Transistor". The Rumennik device includes a drain region having a first portion that extends through the epitaxial layer and extends perpendicularly to connect to the substrate and a second portion that extends laterally along a top surface of the device. The device has a low specific on-resistance and supports high current flow. However, the breakdown voltage of the device is highly dependent on the position of the first portion of the drain region, which narrows the manufacturing tolerance of the device.
對於一展現改善之裝置效能(Rds ,on 與Cgd)與改善之可製造性的橫向擴散金屬氧化物半導體設計仍有所需求。There is still a need for a laterally diffused metal oxide semiconductor design that exhibits improved device performance (R ds , on and Cgd ) and improved manufacturability.
所提供之一種橫向擴散金屬氧化物半導體裝置,其包括一具有一第一導電率類型之基板以及一於其上並具有一上表面之輕度摻雜磊晶層。該第一導電率類型之源極與汲極區域係形成於與該上表面相鄰之磊晶層中,且該等源極與汲極區域係彼此間隔開,並於該磊晶層中具有形成於其間之第二導電率類型的通道區域,同時該通道區域會在該源極區域下延伸。一導電閘極係於一在該通道區域之上形成的閘極介電層上形成,且會部分地重疊該等源極與汲極區域。一汲極接點會使該汲極區域電連接至該基板且係與該通道區域間隔開,其包括一第一溝渠,其從該磊晶層之上表面至該基板而形成,且具有一沿該磊晶層之側壁、一沿該第一溝渠側壁而形成之第一導電率類型的高度摻雜區域以及一鄰接該高度摻雜區域之插在該第一溝渠中的汲極。 一源極接點係電連接至該源極區域,並會在該源極區域與該通道區域間提供一電短路。一絕緣層係形成於該導電閘極與該源極接點間。A laterally diffused metal oxide semiconductor device is provided comprising a substrate having a first conductivity type and a lightly doped epitaxial layer thereon having an upper surface. The source and drain regions of the first conductivity type are formed in an epitaxial layer adjacent to the upper surface, and the source and drain regions are spaced apart from each other and have the epitaxial layer A channel region of a second conductivity type formed therebetween while the channel region extends below the source region. A conductive gate is formed over a gate dielectric layer formed over the channel region and partially overlaps the source and drain regions. A drain contact electrically connects the drain region to the substrate and is spaced apart from the channel region, and includes a first trench formed from an upper surface of the epitaxial layer to the substrate and having a A highly doped region of a first conductivity type formed along a sidewall of the epitaxial layer, a sidewall along the first trench sidewall, and a drain inserted in the first trench adjacent to the highly doped region. A source contact is electrically connected to the source region and provides an electrical short between the source region and the channel region. An insulating layer is formed between the conductive gate and the source contact.
於一替代性具體實施例中,該汲極接點包括一高度摻雜汲極接點區域,其形成於該基板與半導體層中之汲極延伸區域間,其中該高度摻雜汲極接點區域之一最頂部分係與該半導體層之上表面間隔開。一源極接點使該源極區域電耦合至主體區域。In an alternative embodiment, the gate contact includes a highly doped gate contact region formed between the substrate and a drain extension region in the semiconductor layer, wherein the highly doped gate contact One of the topmost portions of the region is spaced apart from the upper surface of the semiconductor layer. A source contact electrically couples the source region to the body region.
從結合附圖的以下本發明之較佳具體實施例的詳細說明將更佳地瞭解本發明之上述與其他特徵。The above and other features of the present invention will be more fully understood from the detailed description of the preferred embodiments of the invention.
當於本文中運用時,以下摻雜物濃度係運用以下符號加以區別:(a)N++或P++:摻雜物濃度約>5x1019 atoms/cm3 ;(b)N+或P+:摻雜物濃度約為1x1018 至5x1019 atoms/cm3 ;(c)N或P:摻雜物濃度約為5x1016 至1x1018 atoms/cm3 ;(d)N-或P-:摻雜物濃度約為1x1015 至5x1016 atoms/cm3 ;以及(e)N--或P--:摻雜物濃度約<1x1015 atoms/cm3 。As used herein, the following dopant concentrations are distinguished by the following notation: (a) N++ or P++: dopant concentration > 5x10 19 atoms/cm 3 ; (b) N+ or P+: dopant concentration Approximately 1x10 18 to 5x10 19 atoms/cm 3 ; (c) N or P: a dopant concentration of about 5 x 10 16 to 1 x 10 18 atoms/cm 3 ; (d) N- or P-: dopant concentration is about 1x10 15 to 5x10 16 atoms/cm 3 ; and (e) N-- or P--: a dopant concentration of about <1x10 15 atoms/cm 3 .
在以下說明中,載述許多特定細節,如材料類型、摻雜量、結構特徵、處理步驟等,以便能對本發明瞭解透徹。熟悉本技術人士將瞭解,可在沒有此等細節中之大部分的情況下實施本文中所說明之本發明。於其他例項中,並無詳細說明熟知之元件、技術、特徵與處理步驟以避免使本 發明難瞭解。In the following description, numerous specific details are set forth, such as material type, doping amount, structural features, processing steps, and the like, in order to provide a thorough understanding of the present invention. Those skilled in the art will appreciate that the invention described herein can be practiced without a substantial portion of the details. In other examples, well-known components, techniques, features, and processing steps are not described in detail to avoid The invention is difficult to understand.
亦應瞭解該等圖式中之元件係代表性且為求明白而沒有依比例繪製。亦應明白,可藉由使所有說明之擴散/摻雜區域均利用相反導電率類型來實現p-通道電晶體。It is also to be understood that the elements in the drawings are representative and are not intended to It will also be appreciated that the p-channel transistor can be realized by having all of the illustrated diffusion/doping regions utilize the opposite conductivity type.
圖1說明一項改善的功率電晶體之具體實施例,較明確地為一改善的橫向擴散金屬氧化物半導體電晶體10。於示範性應用中,該電晶體10係用作為在對如一伺服器或桌上型電腦之電力供應電壓調節器中或在一普遍使用之DC/DC轉換器中的一切換器。1 illustrates a specific embodiment of an improved power transistor, more specifically an improved laterally diffused metal oxide semiconductor transistor 10. In an exemplary application, the transistor 10 is used as a switch in a power supply voltage regulator such as a server or desktop computer or in a commonly used DC/DC converter.
更加明確地說,圖1顯示一改善的n-通道橫向擴散金屬氧化物半導體裝置。該電晶體結構10包括一半導體基板12,其在所說明之具體實施例中,較佳地係一例如與砷或磷進行摻雜的高度摻雜(N+)矽晶圓。高度摻雜(N+)基板具有比P+基板低的電阻,儘管於替代性具體實施例中,該基板12可為P+摻雜。於若干具體實施例中,一汲極電極11係沿該基板12之底部而形成並電連接至該N+基板12。以此方式金屬化該基板12之底部表面有利於未來與一封裝電極(未顯示)之連接有幫助。於一示範性具體實施例中,基板12具有一小於或等於約3密爾(76.2 μm)之厚度,從而對該汲極電極提供一很低電阻接點,並使該基板對該電晶體之導通電阻的影響降至最低。該基板可研磨及/或蝕刻成,或不然形成此所需的厚度。此等程序通常將會在接近該基板晶圓程序之最後方完成。More specifically, Figure 1 shows an improved n-channel laterally diffused metal oxide semiconductor device. The transistor structure 10 includes a semiconductor substrate 12, which in the illustrated embodiment is preferably a highly doped (N+) germanium wafer doped with, for example, arsenic or phosphorous. The highly doped (N+) substrate has a lower electrical resistance than the P+ substrate, although in alternative embodiments the substrate 12 may be P+ doped. In some embodiments, a drain electrode 11 is formed along the bottom of the substrate 12 and electrically connected to the N+ substrate 12. Metallizing the bottom surface of the substrate 12 in this manner facilitates future connections to a packaged electrode (not shown). In an exemplary embodiment, the substrate 12 has a thickness of less than or equal to about 3 mils (76.2 μm) to provide a very low resistance contact to the gate electrode and to cause the substrate to be bonded to the transistor. The effect of on-resistance is minimized. The substrate can be ground and/or etched or otherwise formed to the desired thickness. These procedures will typically be completed near the end of the substrate wafer process.
一輕度摻雜矽磊晶層14係形成於該基板12之上,並具有 一上表面15。於某些具體實施例中,該磊晶層14可具有N(砷或磷)或P(硼)摻雜物類型之摻雜物以及一N-、N--、P-或P--之摻雜物濃度。於一項具體實施例中,該磊晶層具有一介於約1.5至3.5 μm間的厚度。A lightly doped germanium epitaxial layer 14 is formed on the substrate 12 and has An upper surface 15. In some embodiments, the epitaxial layer 14 can have a dopant of the N (arsenic or phosphorous) or P (boron) dopant type and an N-, N-, P- or P-- Dopant concentration. In a specific embodiment, the epitaxial layer has a thickness of between about 1.5 and 3.5 μm.
該磊晶層之摻雜通常係比植入源極/汲極區域的摻雜濃度低。另一方面,於具有垂直電流之裝置情況中,該磊晶層之背景摻雜為了降低於該汲極與該源極間的導通電阻(Rds,on)較佳地係儘可能地高,同時並剛好夠低以滿足該電晶體之目標崩潰電壓。然而,具有本裝置之情況下,由於電流會流過該垂直汲極接點區域22,且該摻雜濃度可維持很低,例如低於2x1016 atoms/cm3 ,且更佳地則等於或低於8x1015 atoms/cm3 ,故而該磊晶層之原始摻雜對於該裝置的電阻便無所影響。The doping of the epitaxial layer is typically lower than the doping concentration of the implanted source/drain regions. On the other hand, in the case of a device having a vertical current, the background doping of the epitaxial layer is preferably as high as possible in order to reduce the on-resistance (Rds, on) between the drain and the source. And just enough low to meet the target breakdown voltage of the transistor. However, with the present device, since current will flow through the vertical drain contact region 22, and the doping concentration can be maintained low, for example, less than 2x10 16 atoms/cm 3 , and more preferably equal to or Below 8x10 15 atoms/cm 3 , the original doping of the epitaxial layer has no effect on the resistance of the device.
一導電閘極31重疊在該磊晶層14之上表面15上。於圖1所說明之具體實施例中,該導電閘極31包括一較低摻雜多晶矽層30,其具有一藉由為熟悉本技術人士所熟知的程序而形成於其中或其上之上矽化物層32。矽化物層32可包括任何過渡金屬矽化物,且於示範性具體實施例中係選自由Ti、W以及Co組成之群。該導電閘極較佳地具有一介於約0.3至0.6 μm間之厚度,以及一由用於其製造之技術生產所界定的長度,例如0.8 μm、0.5 μm、0.35 μm或0.25 μm等。該導電閘極31係於一閘極介電質36上形成,其較佳地包括形成達一介於約150至500之厚度的SiO2 。A conductive gate 31 is overlaid on the upper surface 15 of the epitaxial layer 14. In the embodiment illustrated in FIG. 1, the conductive gate 31 includes a lower doped polysilicon layer 30 having a germanium formed thereon or thereon by a procedure well known to those skilled in the art. Object layer 32. The telluride layer 32 can comprise any transition metal halide, and in an exemplary embodiment is selected from the group consisting of Ti, W, and Co. The conductive gate preferably has a thickness of between about 0.3 and 0.6 μm, and a length defined by the technique for its manufacture, such as 0.8 μm, 0.5 μm, 0.35 μm or 0.25 μm. The conductive gate 31 is formed on a gate dielectric 36, which preferably includes forming a level of between about 150 and 500. The thickness of SiO 2 .
汲極區域20係完全形成於磊晶層14內,並形成一增強的 汲極漂移區域。該增強的汲極漂移區域20係緊靠著或至少相鄰於磊晶層14之上表面15而形成,並且在所說明之具體實施例中具有一摻雜物濃度N。該增強的汲極漂移區域20會提升該橫向擴散金屬氧化物半導體結構10之汲極至源極崩潰電壓。汲極漂移區域20具有一介於約0.5至1.5 μm間之橫向尺寸,以及一介於約0.2至0.4 μm間之深度。該區域20較佳地會於導電閘極之下(即,為該導電閘極所重疊)延伸介於約0.05至0.15 μm間,並且在如Kwon等人之美國專利第5,907,173號之文獻中已知係輕度摻雜汲極(LDD)結構,其全部係以提及方式併入本文之中。The drain region 20 is completely formed in the epitaxial layer 14 and forms an enhanced Bungee drift area. The enhanced drain drift region 20 is formed against or at least adjacent to the upper surface 15 of the epitaxial layer 14, and has a dopant concentration N in the illustrated embodiment. The enhanced drain drift region 20 enhances the drain-to-source breakdown voltage of the laterally diffused metal oxide semiconductor structure 10. The drain drift region 20 has a lateral dimension between about 0.5 and 1.5 μm and a depth between about 0.2 and 0.4 μm. The region 20 preferably extends between the conductive gates (i.e., the conductive gates overlap) between about 0.05 and 0.15 μm, and is disclosed in the literature of U.S. Patent No. 5,907,173 to Kwon et al. Lightly doped drain (LDD) structures are known, all of which are incorporated herein by reference.
該橫向擴散金屬氧化物半導體結構10亦包括一具有一導電率N+之源極植入區域18,其與增強的汲極漂移區域20間隔開。源極區域18會橫向延伸介於約0.5至0.8 μm間,具有一介於約0.15至0.3 μm間之深度,且亦會部分地位於導電閘極之下方介於約0.05至0.15 μm間之處。一具有P-型摻雜物且具有一P濃度導電率之主體區域16係形成於磊晶層14中,並於該源極18與該增強的汲極區域20間具有一次區域,同時於其間形成一通道區域。該主體區域16包括主體接點區域26。於示範性具體實施例中,該主體區域16係形成達一介於約0.5至1.0 μm間之深度,以及水平長度介於約0.8至1.5 μm之間。The laterally diffused metal oxide semiconductor structure 10 also includes a source implant region 18 having a conductivity N+ that is spaced apart from the enhanced drain drift region 20. The source region 18 extends laterally between about 0.5 and 0.8 μm, has a depth of between about 0.15 and 0.3 μm, and is also partially located between the conductive gates and between about 0.05 and 0.15 μm. A body region 16 having a P-type dopant and having a P concentration conductivity is formed in the epitaxial layer 14 and has a region between the source electrode 18 and the enhanced drain region 20 while Form a channel area. The body region 16 includes a body contact region 26. In an exemplary embodiment, the body region 16 is formed to a depth of between about 0.5 and 1.0 μm and a horizontal length of between about 0.8 and 1.5 μm.
該主體接點區域26具有一比該主體區域16之濃度大的摻雜物濃度P++。於一項具體實施例中,該主體接點區域26係形成於一淺溝渠區域19之基底處,並具有一橫向尺寸介 於約0.1至0.3 μm間,且係形成達一介於約0.1至0.3 μm間之深度。該主體接點區域26於源極金屬層28(以下將作較詳細的說明)與該主體區域16間提供一低電阻接點。在其中對該汲極電極施加電壓會使該主體至汲極PN-接面產生一反向偏壓的阻擋情形下,空乏層或區域係在接點植入26與來自該基板12之摻雜梯度間受到垂直方向之"擠壓"。該空乏層之寬度的減少會導致一較低源極-汲極崩潰電壓,其會位於該崩潰發生於該接點植入之下的地方。接著,以上所述會定義用於突崩情形期間所產生之電流的路徑,其中該突崩情形即該主體至汲極PN-接面處之電場極高,因而導致藉由碰撞游離產生少數載子時。The body contact region 26 has a dopant concentration P++ that is greater than the concentration of the body region 16. In a specific embodiment, the body contact region 26 is formed at the base of a shallow trench region 19 and has a lateral dimension. It is between about 0.1 and 0.3 μm and is formed to a depth of between about 0.1 and 0.3 μm. The body contact region 26 provides a low resistance contact between the source metal layer 28 (described in greater detail below) and the body region 16. In the case where a voltage is applied to the drain electrode to cause a reverse bias of the body to the drain PN- junction, the depletion layer or region is implanted at the junction 26 and doped from the substrate 12. The gradient is "squeezed" in the vertical direction. The reduction in the width of the depletion layer results in a lower source-drainage breakdown voltage that would be where the collapse occurred below the junction implant. Next, the above will define a path for the current generated during the sag situation, wherein the sag condition is that the electric field at the PN-junction of the body is extremely high, thereby causing a minority load to be generated by collision. Child time.
一深溝渠區域25(所顯示係由一插塞24所填充)係鄰接增強的汲極漂移區域20並與導電閘極31分隔開而形成。該溝渠25係從該磊晶層14之上表面15至該基板12之上表面而形成。該溝渠25使垂直汲極接點區域22能夠鄰接溝渠區域25之側壁而形成,其會在該增強的汲極漂移區域20與基板12間提供一低電阻路徑,且該低電阻路徑因此達該汲極電極11。於圖1所顯示之n通道具體實施例中,該汲極接點22具有一摻雜物濃度N+或更高,且係在溝渠25開啟的同時藉由低角度植入而形成。溝渠25隨後係以一導電材料(例如,鎢或摻雜多晶矽)或絕緣材料(例如,Six Oy )加以填充而形成插塞24。於一項具體實施例中,汲極接點22會以總量約0.4至0.8 μm之水平尺寸進入磊晶層14中。於其他具體實施例中,該磊晶層係很薄(例如,1.5 μm)且不需要蝕刻該溝 渠以形成汲極接點植入22。於此具體實施例中,該汲極接點22係由第一導電率類型之(若干)擴散區域產生,其藉由多重植入而產生,同時並從該表面延伸至該基板。於此具體實施例中,由於無形成任何的深溝渠25,故而無須汲極插塞。A deep trench region 25 (shown by a plug 24) is formed adjacent to the enhanced drain drift region 20 and spaced apart from the conductive gate 31. The trench 25 is formed from the upper surface 15 of the epitaxial layer 14 to the upper surface of the substrate 12. The trench 25 is formed such that the vertical drain contact region 22 can be adjacent to the sidewall of the trench region 25, which provides a low resistance path between the enhanced drain drift region 20 and the substrate 12, and the low resistance path thus reaches The drain electrode 11. In the n-channel embodiment shown in FIG. 1, the drain contact 22 has a dopant concentration N+ or higher and is formed by low angle implantation while the trench 25 is open. The trench 25 is then filled with a conductive material (e.g., tungsten or doped polysilicon) or an insulating material (e.g., Si x O y ) to form the plug 24. In one embodiment, the drain contact 22 enters the epitaxial layer 14 in a total size of about 0.4 to 0.8 μm. In other embodiments, the epitaxial layer is very thin (eg, 1.5 μm) and does not need to be etched to form the drain contact implant 22. In this particular embodiment, the drain contact 22 is created by a diffusion region (s) of a first conductivity type that is created by multiple implantations while extending from the surface to the substrate. In this embodiment, since no deep trenches 25 are formed, there is no need for a drain plug.
該裝置10亦包括一絕緣層34,其形成於該磊晶層之上表面15之上,且因此於源極植入區域18之上,於該導電閘極31之側壁以及其上表面之上,以及該增強的汲極漂移區域20與接觸插塞24之上。該絕緣層34較佳地包括SiO2 或SiOx Ny 。然而,應瞭解,絕緣層34可包括數層共同形成該絕緣層34的絕緣材料。絕緣層34較佳地係於該導電閘極31之側壁上形成達一至少0.03 μm之厚度,而在該導電閘極31之頂表面上形成達一至少0.05 μm之厚度。於一示範性具體實施例中,絕緣層34係於該汲極區域20上形成達一介於約0.05至0.15 μm之厚度。該絕緣層會使該等汲極區域20與該閘極31與該源極金屬層28絕緣,以下將有所說明。The device 10 also includes an insulating layer 34 formed over the upper surface 15 of the epitaxial layer, and thus over the source implant region 18, over the sidewalls of the conductive gate 31 and above its upper surface. And the enhanced drain drift region 20 and the contact plug 24. The insulating layer 34 preferably comprises SiO 2 or SiO x N y . However, it should be understood that the insulating layer 34 can include a plurality of layers of insulating material that collectively form the insulating layer 34. The insulating layer 34 is preferably formed on the sidewall of the conductive gate 31 to a thickness of at least 0.03 μm, and a top surface of the conductive gate 31 is formed to a thickness of at least 0.05 μm. In an exemplary embodiment, the insulating layer 34 is formed on the drain region 20 to a thickness of between about 0.05 and 0.15 μm. The insulating layer insulates the drain regions 20 from the gate 31 and the source metal layer 28, as will be described below.
如同圖1中所顯示,裝置10亦包括一源極金屬層28,其較佳地包括選自由Al、Ti/Al、Ti/TiN/Al或W組成之群組藉由例如CVD(化學汽相沈積)或濺鍍而毯覆沈積於該裝置上的導電材料。所沈積之源極金屬層28係欲填充淺溝渠19,進而於一源極電極與該源極植入18間提供一接點,同時於該等源極區域18與該主體區域16間提供一短路。源極金屬層28會於絕緣層34上、該導電閘極31上以及該汲極植入區域20與汲極插塞24上延伸。於一項具體實施例中,該源極 金屬層28具有一界定於該磊晶層14之上表面15與其之上表面29間的厚度,其介於約1.0至5.0 μm之間。As shown in FIG. 1, device 10 also includes a source metal layer 28, which preferably includes a group selected from the group consisting of Al, Ti/Al, Ti/TiN/Al, or W by, for example, CVD (Chemical Vapor Phase) Depositing or sputtering to blanket the conductive material deposited on the device. The deposited source metal layer 28 is intended to fill the shallow trench 19, thereby providing a contact between a source electrode and the source implant 18, and providing a source between the source region 18 and the body region 16. Short circuit. The source metal layer 28 extends over the insulating layer 34, the conductive gate 31, and the drain implant region 20 and the drain plug 24. In a specific embodiment, the source The metal layer 28 has a thickness defined between the upper surface 15 of the epitaxial layer 14 and its upper surface 29, which is between about 1.0 and 5.0 μm.
當該橫向擴散金屬氧化物半導體電晶體裝置10係"開啟"時,該導電電流會流過該源極金屬28,橫向地穿透該閘極31之下的通道而至該汲極區域20,且隨後會沿著垂直、高度摻雜汲極接點22,垂直穿透該基板12而至位於該裝置10之底側的汲極電極11。When the laterally diffused metal oxide semiconductor transistor device 10 is "on", the conductive current flows through the source metal 28 and laterally penetrates the channel below the gate 31 to the drain region 20, The gate electrode 12 is then vertically and highly doped, and the substrate 12 is vertically penetrated to the gate electrode 11 on the bottom side of the device 10.
圖1之源極金屬結構28提供許多優點。首先,一單一金屬層可作為一源極接點以及一遮蔽電極,其會遮蔽該導電閘極而與該汲極接點22隔開,並會降低該閘極與該汲極間之電容(Cgd)。無須形成一單獨的遮蔽閘極,亦無須單獨將該遮蔽閘極連接至該源極。從而大幅改善該裝置之可製造性。The source metal structure 28 of Figure 1 provides a number of advantages. First, a single metal layer can serve as a source contact and a shield electrode that shields the conductive gate from the drain contact 22 and reduces the capacitance between the gate and the drain ( Cgd). It is not necessary to form a separate shielding gate, and it is not necessary to separately connect the shielding gate to the source. Thereby the manufacturability of the device is greatly improved.
此外,汲極-源極電阻(Rsd)係藉由運用一N+基板而最佳化。如同熟悉本技術人士將明白,因為於該晶粒底部具有處於接地電位之源極電極係十分重要,所以設計用於RF應用之n-通道裝置通常係形成於P+基板上。儘管n-通道裝置由於其與p-通道裝置相比較低的通道電阻可能較佳,然而先前技術之P-摻雜基板卻提供比n-基板高許多的電阻,通常高出2至3倍。然而,本裝置10會提供一n-通道裝置於一低電阻n-摻雜基板上。In addition, the drain-source resistance (Rsd) is optimized by using an N+ substrate. As will be appreciated by those skilled in the art, n-channel devices designed for RF applications are typically formed on a P+ substrate because of the importance of having a source electrode system at ground potential at the bottom of the die. While n-channel devices may be preferred due to their lower channel resistance compared to p-channel devices, prior art P-doped substrates provide much higher resistance than n-substrate, typically 2 to 3 times higher. However, the device 10 provides an n-channel device on a low resistance n-doped substrate.
現將說明一種形成裝置10之示範性方法。某些對於該等熟悉本技術人士已然清楚之細節將予以摒除,以免使本發明模糊不清。基板12具有一預定義之N+摻雜物濃度。具有 N-或P-摻雜物濃度之磊晶層14接著係於該基板12之上表面上形成。一第一溝渠係在沈積並圖案化一薄氧化物層後蝕刻穿透該磊晶層,以用作為一專用汲極接點遮罩。該溝渠之側壁係具有一合適摻雜物之7度植入的N+摻雜以形成該等汲極接點區域,其中該摻雜物較佳地為磷或砷。該第一溝渠係填充一材料而形成汲極插塞。於一項具體實施例中,該溝渠係填充N+摻雜多晶矽。接著,回蝕該多晶矽至一稍低於該磊晶層之表面的位準,並移除氧化物遮罩。An exemplary method of forming device 10 will now be described. Certain details that are apparent to those skilled in the art will be eliminated so as not to obscure the invention. Substrate 12 has a predefined N+ dopant concentration. have An epitaxial layer 14 of N- or P-dopant concentration is then formed on the upper surface of the substrate 12. A first trench is etched through the epitaxial layer after depositing and patterning a thin oxide layer for use as a dedicated drain contact mask. The sidewalls of the trench are N+ doped with a suitable implant of 7 degrees to form the drain contact regions, wherein the dopant is preferably phosphorus or arsenic. The first trench is filled with a material to form a drain plug. In one embodiment, the trench is filled with N+ doped polysilicon. Next, the polysilicon is etched back to a level slightly below the surface of the epitaxial layer, and the oxide mask is removed.
在於該磊晶層14中形成該汲極接點與該等插塞區域之後,一薄閘極氧化物層係於該磊晶層之上表面15上形成。接著,沈積並蝕刻一多晶矽層以形成一多晶矽閘極。矽化物層32隨後係運用熟知的自對準矽化物程序而形成,或於該多晶矽層上沈積一矽化物層,且隨即加以蝕刻以形成圖1中所顯示之堆疊多晶矽/矽化物結構。接著在形成矽化物層32之後,P-主體或N-增強的漂移區域係藉由個別摻雜物之遮蔽式植入與熱擴散步驟而形成。鄰接該導電閘極之側壁間隔物若需要可運用一已知的側壁間隔物程序而單獨形成。例如,可沈積一氧化物層,然後藉由一非等向性反應離子蝕刻(RIE)回蝕該氧化物層。N+源極區域係藉由運用一圖案化光阻作為一遮罩植入砷而形成。After the gate contact and the plug regions are formed in the epitaxial layer 14, a thin gate oxide layer is formed on the epitaxial layer upper surface 15. Next, a polysilicon layer is deposited and etched to form a polysilicon gate. The telluride layer 32 is then formed using a well-known self-aligned germanide process, or a germanide layer is deposited on the polysilicon layer and then etched to form the stacked polysilicon/germanide structure shown in FIG. Subsequent to the formation of the vaporized layer 32, the P-body or N-enhanced drift region is formed by a masked implantation and thermal diffusion step of individual dopants. The sidewall spacers adjacent the conductive gate can be formed separately using a known sidewall spacer procedure if desired. For example, an oxide layer can be deposited and then etched back by an anisotropic reactive ion etching (RIE). The N+ source region is formed by implanting arsenic as a mask using a patterned photoresist.
一氧化物層34係於該上表面15與導電閘極31之上沈積達所需厚度。接著,淺溝渠19係經圖案化並蝕刻至所需深度,接著並形成植入區域26。最後,一金屬層係於整體結構上進行沈積以形成源極金屬層28。隨後薄化該原始結構 至一所需厚度,並沈積一背側金屬層11以形成該汲極電極。隨後,封裝並測試該裝置。An oxide layer 34 is deposited over the upper surface 15 and the conductive gate 31 to a desired thickness. Next, the shallow trench 19 is patterned and etched to the desired depth, and then the implanted region 26 is formed. Finally, a metal layer is deposited over the monolithic structure to form the source metal layer 28. Thinning the original structure To a desired thickness, a backside metal layer 11 is deposited to form the drain electrode. Subsequently, the device was packaged and tested.
圖2說明一項經改善的橫向擴散金屬氧化物半導體裝置之第二具體實施例10A。該裝置10A就所有方面而言係與圖1之裝置10相同,且相似特徵係以相似參考編碼加以指明,經修改的絕緣層34A與經修改的源極金屬層28A除外。應瞭解,源極金屬層28A之修改僅止於將其沈積於經修改的絕緣層34A上。在與該汲極植入區域20與汲極插塞24相鄰之區域中,經修改的絕緣層34A具有兩厚度。更明確地說,經修改的絕緣層34A具有一通常以35加以指稱之較厚區域,其形成於汲極插塞24與部分的汲極區域20之上,而一較薄部分37則形成於汲極區域20之上,並介於較厚部分35與該閘極31之間。於一項具體實施例中,較薄氧化物區域37之長度的量會達介於該閘極31與該汲極插塞24間之距離的至。於一示範性具體實施例中,較薄部分37之厚度係介於約0.05至0.15 μm間,而較厚部分35之厚度係介於約0.2至0.5 μm間。可先藉由蝕刻在形成該汲極插塞區域後沈積之較厚的氧化物層來形成經改善之絕緣層34A。在閘極形成後沈積該較薄氧化物區域37,且其厚度係添加至該區域34A的最終厚度,其包括部分35。Figure 2 illustrates a second embodiment 10A of an improved laterally diffused metal oxide semiconductor device. The device 10A is identical in all respects to the device 10 of Figure 1, and similar features are indicated by similar reference codes, with the exception of the modified insulating layer 34A and the modified source metal layer 28A. It will be appreciated that the modification of source metal layer 28A is only limited to deposition on modified insulating layer 34A. In the region adjacent the drain implant region 20 and the drain plug 24, the modified insulating layer 34A has two thicknesses. More specifically, the modified insulating layer 34A has a thicker region, generally designated 35, formed over the drain plug 24 and a portion of the drain region 20, and a thinner portion 37 is formed over Above the drain region 20, between the thicker portion 35 and the gate 31. In one embodiment, the length of the thin oxide region 37 may be between the gate 31 and the drain plug 24. to . In an exemplary embodiment, the thinner portion 37 has a thickness between about 0.05 and 0.15 μm, and the thicker portion 35 has a thickness between about 0.2 and 0.5 μm. The improved insulating layer 34A can be formed by etching a thicker oxide layer deposited after forming the drain plug region. The thin oxide region 37 is deposited after the gate is formed and its thickness is added to the final thickness of the region 34A, which includes the portion 35.
圖2之具體實施例中,該源極金屬層28A不僅提供一對該源極區域18與該主體區域16之接點以及一介於該閘極31與該汲極接點22間之遮蔽,其亦會使該場板效應的最佳化更好。該較薄氧化物區域37會藉由將該空乏層從介於該主體 區域16與該汲極20間之PN-接面推離而使該場板效應在閘極隅角處非常有效。若該較薄氧化物係橫向延伸而覆蓋該汲極區域20與該汲極插塞24之全部,則一高電場峰值便會位於N-N+汲極接點隅角處。使該氧化物於35處變得較厚會緩和該源極金屬與該汲極接點區域22間的電場。於該場板下之汲極區域的摻雜與長度、介於區域37與35間之氧化物段差位置以及氧化物厚度可就一給定之崩潰電壓目標而最佳化。作為一範例,就一目標崩潰電壓為20 V而言,此部份電晶體之設計可如下:-總閘極至汲極插塞距離為0.8至1.2 μm;-較薄氧化物區域長度為0.5至0.8 μm;-該較薄氧化物區域厚度為0.06至0.1 μm;-較厚氧化物區域厚度為0.2至0.3 μm;以及-該LDD植入之劑量與能量為5x1012 至7x1012 atoms/cm2 與80至150 keV。In the embodiment of FIG. 2, the source metal layer 28A not only provides a pair of contacts between the source region 18 and the body region 16 and a shield between the gate 31 and the gate contact 22, It will also optimize the plate effect of the field. The thin oxide region 37 will be very effective at the gate corner by pushing the depletion layer away from the PN-junction between the body region 16 and the drain 20. If the thinner oxide extends laterally to cover all of the drain region 20 and the drain plug 24, a high electric field peak will be located at the corner of the N-N+ drain contact. Making the oxide thicker at 35 mitigates the electric field between the source metal and the drain contact region 22. The doping and length of the drain region under the field plate, the oxide step position between regions 37 and 35, and the oxide thickness can be optimized for a given breakdown voltage target. As an example, for a target breakdown voltage of 20 V, the design of this part of the transistor can be as follows: - total gate to drain plug distance is 0.8 to 1.2 μm; - thin oxide region length is 0.5 Up to 0.8 μm; - the thinner oxide region has a thickness of 0.06 to 0.1 μm; - the thicker oxide region has a thickness of 0.2 to 0.3 μm; and - the dose and energy of the LDD implant is 5x10 12 to 7x10 12 atoms/cm 2 with 80 to 150 keV.
圖3說明關於圖1或圖2之橫向擴散金屬氧化物半導體裝置的另一替代性具體實施例10B。圖3之裝置10B係與該等裝置10、10A相同,除了以下所列方面之外:減少主體植入區域16B之深度,並於主體區域16B與基板12間提供第一緩衝區域38。於一示範性具體實施例中,第一緩衝區域38包括一矽層,其以P-摻雜物摻雜成一等於或大於該主體區域16B之摻雜物濃度的濃度。該緩衝層38會緊靠垂直汲極接點22之側壁,且較佳地係形成達一介於約0.3至0.6 μm之厚度。於一項具體實施例中,該緩衝層38係藉由將硼深 度植入該磊晶層14中而形成。於來自圖3之具體實施例10B中,此深度植入係在圖案化較厚氧化物34A之後,但在形成該閘極之前執行。該緩衝層38藉由幫助確認該空乏區域在該通道中並沒有到達太遠,而用以抑制文件中所充分記述之短通道效應。FIG. 3 illustrates another alternative embodiment 10B of the laterally diffused metal oxide semiconductor device of FIG. 1 or 2. The device 10B of Figure 3 is identical to the devices 10, 10A except for the following aspects: reducing the depth of the body implant region 16B and providing a first buffer region 38 between the body region 16B and the substrate 12. In an exemplary embodiment, the first buffer region 38 includes a germanium layer doped with a P-dopant to a concentration equal to or greater than the dopant concentration of the body region 16B. The buffer layer 38 will abut the side walls of the vertical drain contact 22 and is preferably formed to a thickness of between about 0.3 and 0.6 μm. In a specific embodiment, the buffer layer 38 is deepened by boron. The implant is formed by implanting the epitaxial layer 14. In the specific embodiment 10B from Figure 3, this deep implant is performed after patterning the thicker oxide 34A, but before forming the gate. The buffer layer 38 serves to suppress short-channel effects sufficiently described in the document by helping to confirm that the depletion region has not reached too far in the channel.
於圖3之具體實施例中,崩潰之位置仍部分根據磊晶層14之厚度,且部分根據該基板12之摻雜濃度。參考圖4之具體實施例10C,該緩衝層38係為較薄的p-緩衝層38C與具有摻雜物濃度N之第二緩衝層40所取代。於此雙重深度植入緩衝構造中,該崩潰位置有利地係位於介於緩衝層38C與緩衝層40間之P-N接面處或其周圍,而使該崩潰位置主要與該磊晶層之厚度與該基板12之摻雜物濃度無關。深度植入N摻雜物(較佳地為磷)以形成該第二緩衝層40係於該程序流程之初始處,沈積該磊晶層14之後執行。In the embodiment of FIG. 3, the location of the collapse is still based in part on the thickness of the epitaxial layer 14, and in part on the doping concentration of the substrate 12. Referring to the specific embodiment 10C of FIG. 4, the buffer layer 38 is replaced by a thinner p-buffer layer 38C and a second buffer layer 40 having a dopant concentration N. In the dual depth implant buffer structure, the collapse location is advantageously located at or around the P-N junction between the buffer layer 38C and the buffer layer 40, such that the collapse location is primarily associated with the epitaxial layer. The thickness is independent of the dopant concentration of the substrate 12. Deep implantation of an N dopant, preferably phosphorous, to form the second buffer layer 40 is performed at the beginning of the program flow, after deposition of the epitaxial layer 14.
圖5說明於圖2裝置之周邊單元處的邊緣終止,故而無顯示任何閘極。該邊緣終止之結構因其會以一確認目標崩潰電壓之方式關閉該P-N接面,故從一設計透視圖看來係重要。所說明之邊緣終止區域會環繞由P-井16所產生之電晶體之作用區。應明白的是一單一晶粒可具有複數個相等電晶體單元,其如上文中所說明的係製造成並聯,並於(例如)一功率切換器中操作成一單一電晶體。如同上文中結合圖2所說明,該源極金屬28A延伸超過該P-井16,並作用為一場板(其在該裝置之此區域中影響該崩潰電壓)。於層28A之場板部分下的絕緣層(同樣參考編碼35來說明)具 有一介於約0.2至0.5 μm間之厚度,其就如同圖2至4中所顯示之絕緣層34A的較厚氧化物部分35。該汲極插塞24係形成於其中形成該電晶體之切割晶粒的邊緣處,或與其中形成該電晶體之切割晶粒的邊緣相鄰,即該晶粒係從於一在該汲極插塞24處或與該汲極插塞24相鄰之晶圓上的鄰接晶粒切割出來。該邊緣終止區域結束於使該電晶體與該切割晶粒邊緣分離的汲極插塞24。所說明之此結構係形成圖2結構的正常結果。Figure 5 illustrates the termination of the edge at the peripheral unit of the device of Figure 2, so that no gate is shown. The edge-terminated structure is important from a design perspective because it closes the P-N junction in a manner that confirms the target breakdown voltage. The illustrated edge termination region will surround the active region of the transistor produced by the P-well 16. It will be appreciated that a single die may have a plurality of equal transistor cells that are fabricated in parallel as explained above and that operate as a single transistor in, for example, a power switch. As explained above in connection with Figure 2, the source metal 28A extends beyond the P-well 16 and acts as a field plate (which affects the breakdown voltage in this region of the device). An insulating layer under the field plate portion of layer 28A (also described with reference to code 35) There is a thickness between about 0.2 and 0.5 μm, which is like the thicker oxide portion 35 of the insulating layer 34A shown in Figures 2 through 4. The drain plug 24 is formed at an edge of the cut crystal grain in which the transistor is formed, or adjacent to an edge of the cut crystal grain in which the transistor is formed, that is, the die is from the drain Adjacent grains on the plug 24 or on the wafer adjacent to the drain plug 24 are cut. The edge termination region ends with a drain plug 24 that separates the transistor from the edge of the dicing die. This structure illustrated forms the normal result of the structure of Figure 2.
於一較佳具體實施例中,該磊晶層之背景摻雜係1x1016 atoms/cm3 ,該P-井16係藉由重疊深度緩衝38(圖3)與主體16植入而形成,並介於該P-井與該汲極插塞間之距離則係1.5 μm。此邊緣終止可支持高於35 V的崩潰電壓。In a preferred embodiment, the background layer of the epitaxial layer is 1×10 16 atoms/cm 3 , and the P-well 16 is formed by implanting the body 16 with the overlap depth buffer 38 ( FIG. 3 ). The distance between the P-well and the bungee plug is 1.5 μm. This edge termination supports a breakdown voltage above 35 V.
於一示範性應用中,經改善的功率橫向擴散金屬氧化物半導體裝置係與複數個其他相似結構裝置並聯製造,並經封裝以於(例如)一DC/DC電壓調節器中用作功率電晶體。In an exemplary application, the improved power laterally diffused metal oxide semiconductor device is fabricated in parallel with a plurality of other similar structural devices and packaged for use as a power transistor in, for example, a DC/DC voltage regulator. .
圖6至10顯示藉由數值模擬所獲得之圖4之20 V裝置10的電特性,其具有一最大崩潰電壓為20 V且最大允許源極至閘極電壓為12 V之1 mm2 作用區,並具有一閘極厚度為300。圖6顯示汲極電流與汲極電壓在Vgs等於2.0、2.5、3.0、4.0以及5.0伏特時所呈現的函數關係。於飽和區域(Vds>1 V)中的持平Ids曲線顯示該電晶體係不受短通道效應影響。Figures 6 to 10 show the electrical characteristics of the 20 V device 10 of Figure 4 obtained by numerical simulation with a maximum breakdown voltage of 20 V and a maximum allowable source-to-gate voltage of 12 V of 1 mm 2 active region. And has a gate thickness of 300 . Figure 6 shows the relationship between the drain current and the drain voltage as Vgs equals 2.0, 2.5, 3.0, 4.0, and 5.0 volts. The flat Ids curve in the saturated region (Vds > 1 V) shows that the electro-crystalline system is not affected by the short channel effect.
圖7顯示汲極電壓為0.1 V時,一具有計算1 mm2 作用區之裝置的電阻與閘極電壓所呈現的函數關係。可見的是 Vgs等於4.5 V時之預計電阻約13 mΩ*mm2 ,而本技術之相似裝置的電阻則高於20 mΩ*mm2 。Figure 7 shows the resistance of a device with a 1 mm 2 active region as a function of gate voltage when the drain voltage is 0.1 V. It can be seen that the expected resistance at a Vgs of 4.5 V is about 13 mΩ*mm 2 , while the resistance of a similar device of the present technology is higher than 20 mΩ*mm 2 .
圖8顯示汲極電壓為5 V時,汲極電流與閘極電壓所呈現的函數關係。可見的是該電晶體之臨限電壓係保持在低於1.5 V之低值,其對功率應用而言有利。相反地,具有短通道長度之現代化功率MOSFET通常會產生一高許多的臨限電壓,其係大於2.2 V以使該裝置不受短通道效應影響。Figure 8 shows the relationship between the drain current and the gate voltage as the drain voltage is 5 V. It can be seen that the threshold voltage of the transistor is kept below a low value of 1.5 V, which is advantageous for power applications. Conversely, modern power MOSFETs with short channel lengths typically produce a much higher threshold voltage, which is greater than 2.2 V to protect the device from short channel effects.
圖9顯示電容Ciss、Coss以及Crss與汲極電壓所呈現的函數關係,其中CiSS係輸入電容(Cgs+Cgd)、Coss係輸出電容(Cds+Cdg)以及Crss係回授電容(Cdg)。Cdg係很接近Cgd,其取決於源極信號所施加至的端點為何,以及於何端點測量回應信號。一般而言,所提出之裝置會具有比市面上可取得產品小的電容。明確地說,該回授電容Crss(大約等於Cgd)係小於現存的相似功率MOSFETS之5倍。Figure 9 shows the capacitance Ciss, Coss, and Crss as a function of the drain voltage, where CiSS is the input capacitance (Cgs+Cgd), the Coss output capacitance (Cds+Cdg), and the Crss feedback capacitance (Cdg). The Cdg system is very close to Cgd, depending on the endpoint to which the source signal is applied, and at what endpoint the response signal is measured. In general, the proposed device will have a smaller capacitance than commercially available products. Specifically, the feedback capacitor Crss (approximately equal to Cgd) is less than five times the existing similar power MOSFETS.
最後,圖10顯示一閘極電荷曲線。從該曲線可見的是一5 V之閘極電壓可藉由使該閘極僅以2.2nC/mm2 進行充電而達成。此係一很低充電,其提供22 mΩ*nC之Rds(Vgs=10 V)*Qg(VS=5 V)之好處的接受圖,而本技術之相似裝置則產生高於50 mΩ*nC之值。Finally, Figure 10 shows a gate charge curve. It can be seen from this curve that a gate voltage of 5 V can be achieved by charging the gate only at 2.2 nC/mm 2 . This is a very low charge, which provides an acceptance of the benefits of Rds (Vgs = 10 V) * Qg (VS = 5 V) of 22 mΩ * nC, while similar devices of the present technology produce above 50 mΩ * nC value.
如上文中所提及,所提供之經改善功率橫向擴散金屬氧化物半導體裝置具有一n-通道電晶體,其於一低電阻N-基板上形成。該裝置會藉由降低對該基板之電阻影響而展現低導通電阻(Rds-on )以及藉由使該等閘極與汲極電極間之靜 電耦合降至最低而展現低Cgd電容。於具體實施例中,該源極接點會於閘極與汲極區域上延伸,從而提供一高電流能力。As mentioned above, the improved power laterally diffused metal oxide semiconductor device is provided with an n-channel transistor formed on a low resistance N-substrate. The device exhibits a low on-resistance (R ds-on ) by reducing the resistance of the substrate and exhibits a low Cgd capacitance by minimizing electrostatic coupling between the gate and the drain electrode. In a specific embodiment, the source contact extends over the gate and drain regions to provide a high current capability.
圖11說明一項改善的功率電晶體之替代性具體實施例,較明確地為一改善的橫向擴散金屬氧化物半導體電晶體10D。於示範性應用中,該電晶體10D係用作為在對如一伺服器或桌上型電腦之電力供應電壓調節器中或在一普遍使用之DC/DC轉換器中的一切換器。Figure 11 illustrates an alternative embodiment of an improved power transistor, more specifically an improved laterally diffused metal oxide semiconductor transistor 10D. In an exemplary application, the transistor 10D is used as a switch in a power supply voltage regulator such as a server or desktop computer or in a commonly used DC/DC converter.
更加明確地說,圖11顯示一改善的n-通道橫向擴散金屬氧化物半導體裝置10D。如上所述,該電晶體結構10D包括一N+摻雜半導體基板12,然而在替代性具體實施例中該基板12可為P+摻雜。於具體實施例中,一汲極電極11係沿該基板12之底部而形成並電連接至該N+基板12。More specifically, Figure 11 shows an improved n-channel laterally diffused metal oxide semiconductor device 10D. As noted above, the transistor structure 10D includes an N+ doped semiconductor substrate 12, although in alternative embodiments the substrate 12 can be P+ doped. In a specific embodiment, a drain electrode 11 is formed along the bottom of the substrate 12 and electrically connected to the N+ substrate 12.
如上所述,一半導體層係形成於基板12之上。於具體實施例中,該半導體層係一形成於基板12之上表面上的輕度摻雜矽磊晶層14。該磊晶層14具有一上表面,其以參考編碼15指稱。基於不與此揭示內容相關之理由在製造時輕度摻雜該磊晶層,隨後並經摻雜以形成所說明之摻雜分佈,如同下文中更詳細之說明。於一項項具體實施例中,該磊晶層14具有一介於約1.5至3.5 μm間的厚度。該磊晶層厚度係稱為成長層之冶金厚度。As described above, a semiconductor layer is formed over the substrate 12. In a specific embodiment, the semiconductor layer is a lightly doped germanium epitaxial layer 14 formed on the upper surface of the substrate 12. The epitaxial layer 14 has an upper surface, which is referred to by reference numeral 15. The epitaxial layer is lightly doped at the time of manufacture based on reasons not related to this disclosure, and then doped to form the illustrated doping profile, as explained in more detail below. In one embodiment, the epitaxial layer 14 has a thickness of between about 1.5 and 3.5 μm. The thickness of the epitaxial layer is referred to as the metallurgical thickness of the grown layer.
該磊晶層14之摻雜通常比植入源極/汲極區域的摻雜濃度低許多。由於電流會流過該垂直汲極接點區域23(以下將說明),故而該磊晶層之原始摻雜對於該裝置的電阻便 無所影響。於一項具體實施例中,初始摻雜濃度可保持很低,(例如)低於2x1016 atoms/cm3 ,且更佳地等於或低於8x1015 atoms/cm3 。一導電閘極堆疊31(上文所說明)重疊於該磊晶層14之上表面15上。The doping of the epitaxial layer 14 is typically much lower than the doping concentration of the implanted source/drain regions. Since current will flow through the vertical drain contact region 23 (described below), the original doping of the epitaxial layer has no effect on the resistance of the device. In a specific embodiment, the initial doping concentration can be kept low, for example, less than 2 x 10 16 atoms/cm 3 , and more preferably equal to or lower than 8 x 10 15 atoms/cm 3 . A conductive gate stack 31 (described above) is overlaid on the upper surface 15 of the epitaxial layer 14.
汲極植入區域20係完全形成於磊晶層14內,並形成一增強的汲極漂移區域(標定為LDD-N)。於本文中,此區域亦稱為一汲極延伸區域。該汲極延伸區域20係緊靠著或至少相鄰於層14之上表面15而形成,並且在所說明之具體實施例中具有一摻雜物濃度N,其係小於高度摻雜源極區域18之摻雜物濃度(N+)。如同熟悉本技術人士將明白,此汲極延伸區域20會增加該橫向擴散金屬氧化物半導體結構10D的汲極至源極崩潰電壓。該LDD延伸區域20具有一介於約0.3至1.5 μm間之橫向尺寸,以及一介於約0.2至0.4μm間之深度,然而此等尺寸會根據該裝置之所需崩潰電壓額定而有所不同。該區域20較佳地於該導電閘極31之下(即,由該導電閘極31所重疊)延伸介於約0.05至0.15 μm之間。The drain implant region 20 is completely formed within the epitaxial layer 14 and forms an enhanced drain drift region (labeled LDD-N). As used herein, this region is also referred to as a bungee extension region. The drain extension region 20 is formed adjacent or at least adjacent to the upper surface 15 of the layer 14, and in the illustrated embodiment has a dopant concentration N that is less than the highly doped source region The dopant concentration of 18 (N+). As will be appreciated by those skilled in the art, this drain extension region 20 increases the drain-to-source breakdown voltage of the laterally diffused metal oxide semiconductor structure 10D. The LDD extension region 20 has a lateral dimension of between about 0.3 and 1.5 μm and a depth of between about 0.2 and 0.4 μm, although such dimensions will vary depending on the desired breakdown voltage rating of the device. The region 20 preferably extends below the conductive gate 31 (i.e., overlapped by the conductive gate 31) by between about 0.05 and 0.15 μm.
該橫向擴散金屬氧化物半導體結構10D亦包括一具有一導電率N+之源極植入區域18,其與增強的汲極漂移區域20間隔開。源極區域18會橫向延伸介於約0.3至0.8 μm間,具有一介於約0.15至0.3 μm間之深度,且亦會部分地位於該導電閘極31之下方介於約0.05至0.15 μm間之處。該閘極31稍重疊源極區域18與汲極區域20於該裝置之通道區域中提供連續導電。The laterally diffused metal oxide semiconductor structure 10D also includes a source implant region 18 having a conductivity N+ that is spaced apart from the enhanced drain drift region 20. The source region 18 extends laterally between about 0.3 and 0.8 μm, has a depth between about 0.15 and 0.3 μm, and is also partially located below the conductive gate 31 between about 0.05 and 0.15 μm. At the office. The gate 31 slightly overlaps the source region 18 and the drain region 20 to provide continuous conduction in the channel region of the device.
一具有P-型摻雜物且具有一P濃度導電率之主體區域16 係形成於磊晶層14中,並於該源極18與該增強的汲極區域20間具有一次區域,同時於其間形成該通道區域。該主體區域16包括主體接點區域26。於示範性具體實施例中,該主體區域16係形成達一介於約0.5至1.0 μm間之深度,以及水平長度介於約0.8至1.5 μm之間。a body region 16 having a P-type dopant and having a P concentration conductivity It is formed in the epitaxial layer 14 and has a primary region between the source 18 and the enhanced drain region 20 while forming the channel region therebetween. The body region 16 includes a body contact region 26. In an exemplary embodiment, the body region 16 is formed to a depth of between about 0.5 and 1.0 μm and a horizontal length of between about 0.8 and 1.5 μm.
該主體接點區域26具有一比該主體區域16之摻雜物濃度大的高摻雜物濃度(如P++)。如上所述,於一項具體實施例中,該主體接點區域26係形成於一形成於磊晶層14中之淺溝渠區域19的基底處,並具有一半寬度橫向尺寸介於約0.1至0.3 μm間(意即屬於一對相鄰單元中之一單元的寬度),以及一介於約0.1至0.3 μm間之深度。該主體接點區域26於該源極金屬層28與該主體區域16間提供一低電阻接點。在其中對該汲極電極施加電壓會使該主體至汲極PN-接面產生一反向偏壓的阻擋情形下,該空乏層或區域係在該接點植入26與來自該N摻雜緩衝層17或該N+摻雜基板12之摻雜梯度間受到垂直方向之"擠壓"(於若干具體實施例中無N-緩衝17)。該空乏層之寬度的減少會導致一較低源極-汲極崩潰電壓,但位於該崩潰發生於該接點植入區域26之下的地方。隨後,以上所述會定義供在突崩情形期間所產生之電流路徑,其中該突崩情形即是在該主體至汲極PN-接面處之電場極高而藉由碰撞電離使少數載子產生時。The body contact region 26 has a high dopant concentration (e.g., P++) that is greater than the dopant concentration of the body region 16. As described above, in one embodiment, the body contact region 26 is formed at a base of the shallow trench region 19 formed in the epitaxial layer 14 and has a half width transverse dimension of between about 0.1 and 0.3. Between μm (meaning the width of one of a pair of adjacent cells), and a depth between about 0.1 and 0.3 μm. The body contact region 26 provides a low resistance contact between the source metal layer 28 and the body region 16. In the case where a voltage is applied to the drain electrode to cause a reverse bias of the body to the drain PN-junction, the depletion layer or region is implanted at the junction 26 and from the N doping The doping gradient of the buffer layer 17 or the N+ doped substrate 12 is "squeezed" in the vertical direction (in the few embodiments there is no N-buffer 17). The reduction in the width of the depletion layer results in a lower source-drainage breakdown voltage, but where the collapse occurs below the junction implant region 26. Subsequently, the above will define the current path for the period of time during the sag, where the electric field at the PN- junction of the body is extremely high and the minority carrier is made by impact ionization. When it is produced.
儘管位於該植入區域26之下的崩潰電壓可能低於沿該汲極延伸區域20之頂表面的崩潰電壓,然而偏移崩潰位置提 供許多好處。第一,在(例如)關閉該電晶體時出現的熱載子係遠離該閘極堆疊31而產生,並改善閘極氧化物36之可靠性。該閘極氧化物之隅角區域處之電場從未到達臨限位準。第二,於若干具體實施例中,可增加該汲極延伸區域之摻雜濃度(使其達"N"植入之摻雜範圍的較高部分),從而降低其橫向電阻並減少對該裝置之Rds,on的任何相關聯影響。可在所觀察到之電荷平衡設計準則係如下所說明時達成1x1017 atoms/cm3 以上之峰值濃度。While the collapse voltage below the implanted region 26 may be lower than the collapse voltage along the top surface of the drain extension region 20, offsetting the collapse location provides a number of benefits. First, the hot carrier that occurs when, for example, the transistor is turned off is generated away from the gate stack 31 and improves the reliability of the gate oxide 36. The electric field at the corner region of the gate oxide never reaches the threshold level. Second, in several embodiments, the doping concentration of the drain extension region can be increased (to a higher portion of the doping range of the "N" implant), thereby reducing its lateral resistance and reducing the device. Any associated effects of Rds, on. A peak concentration of 1 x 10 17 atoms/cm 3 or more can be achieved when the observed charge balance design criteria are as described below.
該電晶體裝置10D亦包括一如上所述之絕緣層34。The transistor device 10D also includes an insulating layer 34 as described above.
如同上所簡述,該裝置包括高度導電區域23,其形成於該磊晶層14中並將該汲極延伸區域20電連接至該導電基板12。於先前技術橫向擴散金屬氧化物半導體電晶體裝置中,該電晶體之崩潰電壓對於該汲極接點之末端邊緣至該閘極31間之分離的任何變化具有高度敏感性。此距離界定該汲極延伸區域之長度並因其涉及該閘極31與該汲極接點兩者之對準容限而在製造程序中可有所不同。該LDD延伸區域長度之變化接著使裝置設計困難最佳化並使製造窗口窄化。As briefly described above, the apparatus includes a highly conductive region 23 formed in the epitaxial layer 14 and electrically connecting the drain extension region 20 to the conductive substrate 12. In prior art laterally diffused metal oxide semiconductor transistor devices, the breakdown voltage of the transistor is highly sensitive to any change in the separation between the end edge of the gate contact and the gate 31. This distance defines the length of the drain extension region and may vary in the manufacturing process as it relates to the alignment tolerance of both the gate 31 and the gate contact. The change in length of the LDD extension region then optimizes device design difficulties and narrows the manufacturing window.
於圖11之裝置的較佳具體實施例中,該導電區域23係一N+摻雜植入區域23,其形成於該基板12與該汲極延伸區域20之間。此摻雜區域23與該閘極31橫向且垂直間隔開。該摻雜區域23之最頂部分亦與該磊晶層14之上表面15垂直間隔開(即,自該磊晶層14之上表面15凹陷)。於若干具體實施例中,摻雜區域23係以該汲極延伸區域20之至少一部分 與該磊晶層14之上表面15間隔開。於若干具體實施例中,該高度摻雜植入區域23可部分延伸至該汲極延伸區域20中,然而於若干較佳具體實施例中其實質上侷限於該汲極延伸區域20與該基板12所界定之區,而僅製造電接點至該汲極延伸區域20。摻雜汲極接點區域23於該汲極延伸區域20與該基板12間提供一低電阻路徑,並因此達該汲極電極11。於圖11所顯示之n-通道具體實施例中,該汲極接點23具有N+或更高的摻雜物濃度。於一項具體實施例中,汲極接點23於磊晶層14中具有一水平寬度達約0.2至0.4 μm之量(半寬度)。In a preferred embodiment of the apparatus of FIG. 11, the conductive region 23 is an N+ doped implant region 23 formed between the substrate 12 and the drain extension region 20. This doped region 23 is laterally and vertically spaced apart from the gate 31. The topmost portion of the doped region 23 is also vertically spaced from the upper surface 15 of the epitaxial layer 14 (i.e., recessed from the upper surface 15 of the epitaxial layer 14). In several embodiments, the doped region 23 is at least a portion of the drain extension region 20 It is spaced apart from the upper surface 15 of the epitaxial layer 14. In some embodiments, the highly doped implant region 23 can extend partially into the drain extension region 20, although in some preferred embodiments it is substantially limited to the drain extension region 20 and the substrate. 12 defined zones, and only electrical contacts are made to the bungee extension zone 20. The doped gate contact region 23 provides a low resistance path between the drain extension region 20 and the substrate 12 and thus reaches the drain electrode 11. In the n-channel embodiment shown in FIG. 11, the drain contact 23 has a dopant concentration of N+ or higher. In one embodiment, the drain contact 23 has a horizontal width in the epitaxial layer 14 of about 0.2 to 0.4 μm (half width).
使用N+摻雜區域23作為該汲極延伸區域20與該基板12間之接點提供許多製造與操作好處。可輕易地將此摻雜分佈施用至低電壓MOSFET,其中該磊晶層14之摻雜的持平部分十分短且量通常介於約0.5至2.5 μm之間。例如,在Vds,max為20 V之所設計n-通道MOSFET之情況中,可藉由兩連續的磷植入來形成該汲極插塞區域23。於此具體實施例中,第一植入於200 keV具有8e12 cm-2 之劑量而第二植入於800 keV具有8e12 cm-2 之劑量。由一厚度約1.3 μm之光阻覆蓋一厚度約1.5 μm之氧化物於該磊晶層14之上表面15之上形成的雙層可遮蔽此等植入。The use of the N+ doped region 23 as a junction between the drain extension region 20 and the substrate 12 provides a number of manufacturing and operational benefits. This doping profile can be readily applied to a low voltage MOSFET where the doped flat portion of the epitaxial layer 14 is very short and typically is between about 0.5 and 2.5 μιη. For example, in the case of an n-channel MOSFET designed with Vds, max of 20 V, the drain plug region 23 can be formed by two consecutive phosphorous implants. In this particular embodiment, the first implant at 200 keV with a dose of 8e12 cm -2 at 800 keV and the second implant has a dose of 8e12 cm -2. A double layer formed by a photoresist having a thickness of about 1.3 μm covering a thickness of about 1.5 μm over the upper surface 15 of the epitaxial layer 14 shields the implants.
該摻雜汲極接點區域23會產生一高導電率區域,其插在該汲極延伸區域20與該磊晶層14之基板12所產生之摻雜分佈之間。此區域之較佳摻雜濃度係至少1x1018 atoms/cm3 。該摻雜汲極接點區域23之重要特徵在於該區 域實質上或完全限制於該汲極延伸區域20之下。此特徵使該電晶體10D之崩潰電壓對該汲極接點與該導電閘極31間之距離變化較不敏感許多,如此改善其製造的處理窗口。如同以下亦說明的,在相較於具有相同崩潰電壓之裝置時,此修改結構使該汲極區域20能設計成具有一較短長度(為原始LDD長度之70%至90%的等級)。接著,如此使得作用單元之間距較小,隨後並使每單位面積之MOSFET之通道密度增加,使該裝置之特定電阻降低(Rds,on*面積)。在無此凹陷設計之情況下,該汲極延伸區域必然較長,使得該汲極接點與該導電閘極橫向間隔開,以便能降低沿該磊晶層表面之高電場。若該汲極接點並未凹陷,則該崩潰會平行於該磊晶層之表面而發生並使該空乏區域經擠壓而接近該磊晶層之表面,且需使長LDD延伸區域能容納該崩潰以便能達到一目標崩潰電壓。在圖11之設計的情況下,該高電場便更加深入該磊晶層,並可觀察到碰撞電離強度之傾斜(例如,約45∘角)梯度。該高電場發生在導電率最高之區域處(即,該凹陷汲極接點區域23而非該汲極區域20)。在相較於具有相同間距之裝置時,如此使設計較輕鬆且崩潰電壓較高(例如,5至7 V或更高)。The doped gate contact region 23 produces a region of high conductivity that is interposed between the drain extension region 20 and the dopant profile produced by the substrate 12 of the epitaxial layer 14. The preferred doping concentration for this region is at least 1 x 10 18 atoms/cm 3 . An important feature of the doped gate contact region 23 is that the region is substantially or completely confined below the drain extension region 20. This feature makes the breakdown voltage of the transistor 10D much less sensitive to changes in the distance between the drain contact and the conductive gate 31, thus improving the processing window of its fabrication. As also explained below, the modified structure allows the drain region 20 to be designed to have a shorter length (a level of 70% to 90% of the original LDD length) compared to a device having the same breakdown voltage. This, in turn, results in a smaller distance between the active cells, which in turn increases the channel density of the MOSFET per unit area, reducing the specific resistance of the device (Rds, on* area). In the absence of such a recessed design, the drain extension region must be relatively long such that the drain contact is laterally spaced from the conductive gate to reduce the high electric field along the surface of the epitaxial layer. If the gate contact is not recessed, the collapse occurs parallel to the surface of the epitaxial layer and the depletion region is squeezed to approach the surface of the epitaxial layer, and the long LDD extension region needs to be accommodated. This crash is such that a target crash voltage can be reached. In the case of the design of Figure 11, the high electric field deepens into the epitaxial layer and a gradient of the impact ionization intensity (e.g., about 45 angstroms) is observed. This high electric field occurs at the region where the conductivity is the highest (i.e., the depressed gate contact region 23 is not the gate region 20). This makes the design easier and the breakdown voltage higher (for example, 5 to 7 V or higher) compared to devices with the same pitch.
於較佳具體實施例中,該橫向擴散金屬氧化物半導體裝置10D之磊晶層14係經摻雜而包括一直接形成於該基板12之上的薄N-摻雜緩衝層17(標定成N-緩衝)。於若干具體實施例中,該緩衝層17之摻雜濃度係與主體區域16之摻雜濃度(即,N摻雜濃度)可比較或比主體區域16之摻雜濃度稍 高。此緩衝區域17係用以壓制該源極接點區域下(即,植入區域26下)之電晶體崩潰電壓,因而抑制該磊晶層厚度的變化對該裝置之效能所產生的影響。In a preferred embodiment, the epitaxial layer 14 of the laterally diffused metal oxide semiconductor device 10D is doped to include a thin N-doped buffer layer 17 directly formed on the substrate 12 (calibrated to N) -buffer). In several embodiments, the doping concentration of the buffer layer 17 is comparable to or less than the doping concentration of the body region 16 (ie, the N doping concentration). high. The buffer region 17 is used to suppress the dielectric breakdown voltage under the source contact region (i.e., under the implant region 26), thereby suppressing the effect of variations in the thickness of the epitaxial layer on the performance of the device.
一P-摻雜緩衝層21係形成於該N-摻雜緩衝17上,該LDD延伸區域20下,並橫向地介於該p-主體16與N+摻雜汲極接點區域23之間。該緩衝層21與該主體區域16係分別進行摻雜,且此層中之片電荷(濃度乘以厚度)係與該LDD層20內之片電荷可比較。以下將更加詳細地討論此緩衝層21。A P-doped buffer layer 21 is formed on the N-doped buffer 17 under the LDD extension region 20 and laterally interposed between the p-body 16 and the N+ doped gate contact region 23. The buffer layer 21 and the body region 16 are doped separately, and the sheet charge (concentration multiplied by the thickness) in the layer is comparable to the sheet charge in the LDD layer 20. This buffer layer 21 will be discussed in more detail below.
該汲極延伸區域20與該緩衝區域21符合如(例如)美國專利第4,754,310號與第5,216,275號中所討論之電荷平衡的設計準則,該等專利之全部係以提及方式併入本文。此電荷平衡技術(亦稱為電荷耦合)會以一交替導電率類型之第一與第二區域的交錯結構取代一傳統電晶體汲極區域之單一高電阻性部分(一般認為該部分會在一空乏層中吸收該裝置之高阻遏電壓)。在崩潰電壓提升之情況下,必須使傳統汲極之漂移區域較長且摻雜較少以便能提升Rds。欲於該裝置結構中達成一所需崩潰電壓,應平衡並最佳化該等區域中之電荷以使崩潰電壓最高且Rds-on最低。此等第一與第二區域中之每一區域之摻雜濃度的厚度使得一旦空乏,於此等區域中之每一區域中形成之每一單位面積的空間電荷便平衡。於本發明之較佳具體實施例中,電荷平衡係提供於該汲極區域20與該P-緩衝區域21之間。該空乏區域會以補償淨電荷在此等兩區域中同時發展,且產生的電場分佈亦十分均勻。此技術使維持該裝置之目標阻遏電壓 所需之距離變較短並使該汲極區域20中之摻雜量變得較高(即,導電率較高)。於若干具體實施例中,該摻雜量增加約10至30倍,而從N-變成N摻雜量。如此使該區域20之電阻降低。The drain extension region 20 and the buffer region 21 conform to the design criteria for charge balancing as discussed in, for example, U.S. Patent Nos. 4,754,310 and 5,216,275, the entireties of each of each of This charge balancing technique (also known as charge coupling) replaces a single high-resistance portion of a conventional transistor's drain region with a staggered structure of the first and second regions of an alternating conductivity type (generally considered to be in one The high repression voltage of the device is absorbed in the depletion layer). In the case of a breakdown voltage increase, the drift region of the conventional drain must be made longer and doped less to increase the Rds. To achieve a desired breakdown voltage in the device structure, the charge in those regions should be balanced and optimized to maximize the breakdown voltage and minimize Rds-on. The thickness of the doping concentration of each of the first and second regions is such that, once depleted, the space charge per unit area formed in each of the regions is balanced. In a preferred embodiment of the invention, a charge balance is provided between the drain region 20 and the P-buffer region 21. The depletion region will develop simultaneously in the two regions with compensated net charge, and the resulting electric field distribution is also very uniform. This technique maintains the target rejection voltage of the device The required distance becomes shorter and the doping amount in the drain region 20 becomes higher (i.e., the conductivity is higher). In several embodiments, the amount of doping is increased by about 10 to 30 times, and from N- to an amount of N doping. This reduces the electrical resistance of the region 20.
N-摻雜緩衝區域17具有一摻雜物濃度N而P-摻雜緩衝區域21具有一摻雜物濃度P。深度植入N摻雜物(較佳地為磷)以形成該緩衝層17可在該程序流程開始時,該磊晶層14沈積之後執行。緩衝層21可在植入層17之後或在形成汲極插塞23之後形成。The N-doped buffer region 17 has a dopant concentration N and the P-doped buffer region 21 has a dopant concentration P. The deep implantation of an N dopant, preferably phosphorous, to form the buffer layer 17 can be performed after deposition of the epitaxial layer 14 at the beginning of the program flow. The buffer layer 21 may be formed after the implant layer 17 or after the formation of the drain plug 23.
裝置10D之源極金屬層或電極28較佳地包括如藉由CVD(化學汽相沈積)或濺鍍而毯覆沈積於該裝置上之選自由Al、Ti/Al、Ti/TiN/Al或W組成之群組的導電材料。該金屬層28可包括多重金屬或金屬合金層。於若干具體實施例中,該源極電極28可經線路接合或直接焊接至外部封裝電極。沈積該源極電極28以填充淺溝渠19,進而提供與該源極植入18之電接觸以及在該源極18與該主體區域16間產生一短路。源極電極28會在絕緣層34之上延伸並覆蓋該晶圓之全部表面區,包括該閘極結構31與該汲極延伸區域20(位處該閘極接點旁邊之小區除外)。於一項具體實施例中,該源極金屬層28具有界定於該磊晶層14之上表面15與其上表面29間之厚度,其介於約1.0至5.0 μm之間。The source metal layer or electrode 28 of device 10D preferably comprises a blanket deposited on the device, such as by Al, Ti/Al, Ti/TiN/Al, or by sputtering by CVD (Chemical Vapor Deposition) or sputtering. A conductive material of the group consisting of W. The metal layer 28 can comprise a plurality of metal or metal alloy layers. In several embodiments, the source electrode 28 can be wire bonded or soldered directly to an external package electrode. The source electrode 28 is deposited to fill the shallow trench 19, thereby providing electrical contact with the source implant 18 and creating a short between the source 18 and the body region 16. The source electrode 28 extends over the insulating layer 34 and covers the entire surface area of the wafer, including the gate structure 31 and the drain extension region 20 (except for the cell adjacent to the gate contact). In one embodiment, the source metal layer 28 has a thickness defined between the upper surface 15 of the epitaxial layer 14 and its upper surface 29, which is between about 1.0 and 5.0 μm.
當該裝置10D係"開啟"時,導電電流會流過該源極金屬28,流過源極區域18,穿透該閘極31之下的通道而橫向流至該汲極延伸區域20,穿透該汲極延伸區域20流至垂直高 度摻雜汲極接點23進而至該基板12,並穿透該基板12而流至該汲極電極11,其係電耦合至該裝置10D之底側。When the device 10D is "on", a conductive current will flow through the source metal 28, through the source region 18, through the channel below the gate 31, and laterally to the drain extension region 20, through Through the drain extension region 20 to the vertical height The gate contact 23 is further doped to the substrate 12 and penetrates the substrate 12 to flow to the drain electrode 11 which is electrically coupled to the bottom side of the device 10D.
圖11之源極金屬結構28提供許多優點。首先,一單一導電層可作為一源極接點以及一遮蔽電極兩者,其會遮蔽該導電閘極31而與該汲極接點23隔開,並會降低該閘極與該汲極間之電容(Cgd)。由於該表面15之下之汲極接點區域23的凹陷,故而該絕緣層34現可具有約等於圖3至4中之較薄部分37之厚度的單一均勻厚度。無任何形成一單獨遮蔽閘極之必要亦無任何將該遮蔽閘極單獨連接至該源極18之必要。從而,大幅改善該裝置之可製造性。The source metal structure 28 of Figure 11 provides a number of advantages. First, a single conductive layer can serve as both a source contact and a shield electrode, which shields the conductive gate 31 from the drain contact 23 and reduces the gate and the drain. Capacitance (Cgd). Due to the depression of the drain contact region 23 below the surface 15, the insulating layer 34 may now have a single uniform thickness approximately equal to the thickness of the thinner portion 37 of Figures 3 through 4. There is no need to form a single shield gate or any separate connection of the shield gate to the source 18. Thereby, the manufacturability of the device is greatly improved.
此外,藉由使用一N+基板12來最佳化汲極-源極電阻(Rds)。即便是先前技術之P-摻雜基板提供比n-基板高許多的電阻(經常高出2至3倍),然而熟悉本技術人士將明白,針對RF應用所設計之n-通道裝置通常係形成於P+基板上,因為於該晶粒底部具有位處接地電位之源極電極係十分重要。然而,本電晶體裝置10D會在一低電阻n-摻雜基板12上提供一n-通道裝置。In addition, the drain-source resistance (Rds) is optimized by using an N+ substrate 12. Even prior art P-doped substrates provide much higher resistance (often 2 to 3 times higher) than n-substrate, however, those skilled in the art will appreciate that n-channel devices designed for RF applications are typically formed. On the P+ substrate, it is important to have a source electrode system with a ground potential at the bottom of the die. However, the present crystal device 10D provides an n-channel device on a low resistance n-doped substrate 12.
於一項具體實施例中,使該源極金屬28與該汲極延伸區域20重疊並利用一預定義厚度之絕緣層34使該等兩區域分離可誘發額外的電荷耦合。於若干具體實施例中,該絕緣層34於此區域中具有一介於約0.05至0.15 μm之厚度。可以數值模擬並最佳化該電場分佈來決定最佳厚度。此電荷耦合效應使該汲極延伸區域20之摻雜濃度再度增加,進而使Rds降低。In one embodiment, the source metal 28 is overlapped with the drain extension region 20 and the two regions are separated by a predetermined thickness of insulating layer 34 to induce additional charge coupling. In some embodiments, the insulating layer 34 has a thickness in this region of between about 0.05 and 0.15 μm. The electric field distribution can be numerically simulated and optimized to determine the optimum thickness. This charge coupling effect causes the doping concentration of the drain extension region 20 to increase again, thereby lowering the Rds.
現將說明一種形成裝置10D之示範性方法。某些對於熟悉本技術人士已然清楚之細節將予以摒除,以免使本發明模糊不清。基板12具有一預定義N+摻雜物濃度。接著,於該基板12之上表面上形成磊晶層14。視需要,在沈積該磊晶層14之後,藉由深度植入N摻雜物(較佳地為磷)來形成N-緩衝層17。於該磊晶層14上形成並圖案化用作一汲極接點遮罩的氧化物層。植入區域23係運用上述之雙植入程序而形成。運用一蝕刻程序移除該氧化物層之部分以如一專用光阻遮罩所界定地揭露該電晶體之作用區。於該電晶體作用區內植入該P-緩衝層21。移除該光阻遮罩並使用剩餘氧化物層作為所謂環繞作用電晶體區而覆蓋該晶粒的場氧化物。An exemplary method of forming device 10D will now be described. Certain details that are apparent to those skilled in the art will be eliminated so as not to obscure the invention. Substrate 12 has a predefined N+ dopant concentration. Next, an epitaxial layer 14 is formed on the upper surface of the substrate 12. The N-buffer layer 17 is formed by deeply implanting an N dopant, preferably phosphorus, after depositing the epitaxial layer 14 as needed. An oxide layer serving as a drain contact mask is formed and patterned on the epitaxial layer 14. The implanted region 23 is formed using the dual implant procedure described above. A portion of the oxide layer is removed using an etch process to expose the active region of the transistor as defined by a dedicated photoresist mask. The P-buffer layer 21 is implanted in the active region of the transistor. The photoresist mask is removed and the remaining oxide layer is used as a so-called surrounding active transistor region to cover the field oxide of the die.
形成該汲極接點23後,於該磊晶層14之上表面15上形成一薄閘極氧化物層36。接著,沈積並蝕刻一多晶矽層以形成一多晶矽閘極層30。矽化物層32隨後係運用熟知的自對準矽化物程序而形成,或於該多晶矽層30上沈積一矽化物層,且隨即加以蝕刻以形成圖11中所顯示之堆疊多晶矽/矽化物結構31。接著在形成矽化物層32之後,該P-主體16與該汲極延伸區域20係藉由個別摻雜物之遮蔽式植入與熱擴散步驟而形成。鄰接該導電閘極31之側壁間隔物若需要可運用一已知側壁間隔物程序而個別地形成。例如,可沈積一氧化物層,然後藉由一非等向的反應離子蝕刻(RIE)回蝕該氧化物層以形成絕緣間隔物。該N+源極區域18係藉由運用一圖案化光阻作為一遮罩植入砷而形成。After the gate contact 23 is formed, a thin gate oxide layer 36 is formed on the upper surface 15 of the epitaxial layer 14. Next, a polysilicon layer is deposited and etched to form a polysilicon gate layer 30. The telluride layer 32 is then formed using a well-known self-aligned germanide process, or a germanide layer is deposited over the polysilicon layer 30 and then etched to form the stacked polysilicon/germanide structure 31 shown in FIG. . Subsequent to the formation of the vaporized layer 32, the P-body 16 and the drain extension region 20 are formed by a masked implantation and thermal diffusion step of individual dopants. The sidewall spacers adjacent to the conductive gate 31 can be individually formed using a known sidewall spacer procedure if desired. For example, an oxide layer can be deposited and then etched back by an anisotropic reactive ion etching (RIE) to form an insulating spacer. The N+ source region 18 is formed by implanting arsenic as a mask using a patterned photoresist.
一氧化物層34係於該上表面15與導電閘極31之上沈積達所需厚度。淺溝渠19係經圖案化並蝕刻至所需深度,接著並形成植入區域26。最後,一金屬層係於整體結構上進行沈積並經圖案化以形成源極金屬28。隨後薄化該原始結構至一所需厚度,並沈積一背側金屬11以形成該汲極電極。隨後,封裝並測試該裝置。An oxide layer 34 is deposited over the upper surface 15 and the conductive gate 31 to a desired thickness. The shallow trench 19 is patterned and etched to the desired depth, and then the implanted region 26 is formed. Finally, a metal layer is deposited over the monolithic structure and patterned to form the source metal 28. The original structure is then thinned to a desired thickness and a backside metal 11 is deposited to form the drain electrode. Subsequently, the device was packaged and tested.
以下說明該電晶體裝置10D之各種其他具體實施例。可運用上述程序以及熟悉本技術人士將明白之本文中未說明之對該程序的修改來形成此等裝置。Various other specific embodiments of the crystal device 10D will be described below. Such devices may be formed using the above-described procedures and modifications to the program that are not apparent to those skilled in the art.
圖12說明一改善之橫向擴散金屬氧化物半導體電晶體10E之具體實施例。該電晶體10E係與上述電晶體10D相同(以下所說明的除外),且相似參考編碼指明相似特徵。於圖12之具體實施例中,該磊晶層14包括以摻雜多晶矽填充之第二溝渠46。高度導電(N+)摻雜之植入區域23A環繞該摻雜多晶矽。多晶矽沈積之後,於一回蝕步驟中使該多晶矽填充溝渠46從該磊晶層14之頂表面15凹陷。於一較佳具體實施例中,就地摻雜該多晶矽。此凹陷係以來自絕緣層34B之介電材料來填充。該多晶矽插塞46係與汲極延伸區域20A相鄰。於此具體實施例中,該導電區域23A係藉由使摻雜物從該摻雜多晶矽材料擴散至該磊晶層14之環繞部分中來形成以電接觸該汲極延伸區域20A與該基板12兩者。擴散會在製造該橫向擴散金屬氧化物半導體電晶體10E時所運用且熟悉本技術人士將熟悉的高溫退火期間發生。退火步驟通常在閘極氧化物形成期間使用及/或用以 活化該主體或源極/汲極區域16、18、20A中的植入摻雜物。環繞該多晶矽填充46產生之N+井23A會形成將該汲極延伸區域20A連接至該基板12的高度導電汲極插塞。由於具有上述之導電汲極接點插塞23,故而此高度摻雜區域23A係如藉由該輕度摻雜區域20A與該絕緣層34B之至少一部分與該磊晶層14之頂表面15間隔開。Figure 12 illustrates a specific embodiment of an improved laterally diffused metal oxide semiconductor transistor 10E. The transistor 10E is identical to the transistor 10D described above (except as explained below), and similar reference codes indicate similar features. In the embodiment of FIG. 12, the epitaxial layer 14 includes a second trench 46 filled with doped polysilicon. A highly conductive (N+) doped implant region 23A surrounds the doped polysilicon. After the polycrystalline germanium is deposited, the polycrystalline germanium filled trench 46 is recessed from the top surface 15 of the epitaxial layer 14 in an etch back step. In a preferred embodiment, the polysilicon is doped in situ. This recess is filled with a dielectric material from insulating layer 34B. The polysilicon plug 46 is adjacent to the drain extension region 20A. In this embodiment, the conductive region 23A is formed by diffusing dopants from the doped polysilicon material into the surrounding portion of the epitaxial layer 14 to electrically contact the drain extension region 20A and the substrate 12. Both. Diffusion occurs during the fabrication of the laterally diffused metal oxide semiconductor transistor 10E and is experienced during high temperature annealing which will be familiar to those skilled in the art. The annealing step is typically used during gate oxide formation and/or Implant dopants in the body or source/drain regions 16, 18, 20A are activated. The N+ well 23A created around the polysilicon fill 46 forms a highly conductive drain plug that connects the drain extension region 20A to the substrate 12. Since the conductive gate contact plug 23 is provided, the highly doped region 23A is spaced apart from the top surface 15 of the epitaxial layer 14 by at least a portion of the lightly doped region 20A and the insulating layer 34B. open.
圖13說明一改善之橫向擴散金屬氧化物半導體電晶體10F之另一具體實施例。該電晶體10F係與上述圖12之電晶體10E相同(以下所說明的除外),且相似參考編碼指明相似特徵。於此具體實施例中,在該N+源極18A與下方P-主體區域16間提供一電短路之源極金屬層28A係以一金屬填充從該磊晶層14之頂表面15穿透該N+源極區域18A所蝕刻之一淺溝渠19A而形成。於此具體實施例中,該源極接點溝渠19A係自對準該導電閘極堆疊31。此自對準方法使布局間距能減小,並使該MOSFET之通道每單位面積之密度增加,因而降低該裝置之特定電阻(Rds,on *面積)。於該自對準程序中,該源極接點遮罩具有至少部分於該導電閘極31上延伸的接點開口,該導電閘極31已事先覆蓋一介電層,該介電層為介電層34C之前導物且於該閘極31頂上具有的厚度與接點區中該磊晶層14之矽表面15上具有的厚度不同。可使用兩沈積來產生具有不同厚度的區域。該閘極結構31頂上之介電層厚度明顯大於該接點區中之介電層厚度,如大於約0.3至0.5 μm,因而該接點蝕刻會在到達該閘極堆疊31之頂表面之前停止在該磊晶層上表面15上或附 近。於接續的步驟中,於該接點區中穿透該N+源極區域18A蝕刻該磊晶層14並達一低於該N+源極區域18A之深度,進而碰到該主體區域16。第二蝕刻步驟使用一蝕刻劑,其對該磊晶層14比對該介電層34C更具選擇性。隨後,在該基板上將形成源極電極28A之金屬層沈積成一連續層,其中該金屬填充該源極接點溝渠19A並重疊該閘極31與汲極延伸區域20A。於此具體實施例中,該源極接點開口大小與形成圖11至12之裝置所使用的開口大小相同,但接點窗口與該閘極堆疊31間之分離則因該重疊而減小。接著,如此在與裝置10至10E相較時該裝置10F之間距便為減小的。Figure 13 illustrates another embodiment of an improved laterally diffused metal oxide semiconductor transistor 10F. The transistor 10F is identical to the transistor 10E of Fig. 12 described above (except as explained below), and similar reference codes indicate similar features. In this embodiment, the source metal layer 28A that provides an electrical short between the N+ source 18A and the lower P-body region 16 penetrates the N+ from the top surface 15 of the epitaxial layer 14 with a metal fill. The source region 18A is formed by etching one of the shallow trenches 19A. In this embodiment, the source contact trench 19A is self-aligned to the conductive gate stack 31. This self-aligned approach reduces the layout pitch and increases the density per channel area of the MOSFET channel, thereby reducing the specific resistance (Rds, on* area) of the device. In the self-aligned process, the source contact mask has a contact opening extending at least partially over the conductive gate 31. The conductive gate 31 has previously covered a dielectric layer, and the dielectric layer is The lead of the electrical layer 34C has a thickness on top of the gate 31 that is different from the thickness of the tantalum surface 15 of the epitaxial layer 14 in the contact region. Two deposits can be used to create regions of different thicknesses. The thickness of the dielectric layer on top of the gate structure 31 is significantly greater than the thickness of the dielectric layer in the contact region, such as greater than about 0.3 to 0.5 μm, so that the contact etch stops before reaching the top surface of the gate stack 31. On the upper surface 15 of the epitaxial layer or attached near. In a subsequent step, the epitaxial layer 14 is etched through the N+ source region 18A in the contact region and reaches a depth lower than the N+ source region 18A, thereby contacting the body region 16. The second etch step uses an etchant that is more selective to the epitaxial layer 14 than to the dielectric layer 34C. Subsequently, a metal layer forming the source electrode 28A is deposited on the substrate as a continuous layer, wherein the metal fills the source contact trench 19A and overlaps the gate 31 and the drain extension region 20A. In this embodiment, the source contact opening is the same size as the opening used to form the device of Figures 11 through 12, but the separation between the contact window and the gate stack 31 is reduced by the overlap. Then, the distance between the devices 10F is reduced as compared to the devices 10 to 10E.
於部分具體實施例中,該源極接點遮罩亦用以在該P-主體區域16中執行遮蔽式P+植入。第一植入係在氧化物蝕刻後執行並在恰於該N+源極區域18A之下方產生一P+區域48。該植入48會降低該N+源極區域18A下方之P-主體16A的片電阻,以便能在突崩潰期間完全避免觸發雙極電晶體作用。第二P++植入26係在蝕刻該磊晶層14以形成溝渠19A之後執行。此植入係用以增加該源極接點28A對該P-主體區域16A之介面處的摻雜濃度,進而改善該源極金屬層28A與該P-主體16A間的接點。在沒有N+緩衝層17之情況下,該突崩潰之位置係固定於植入區域48與N+接點23或23A之間,而非恰固定於該源極接點植入區域26之下方。In some embodiments, the source contact mask is also used to perform a shielded P+ implant in the P-body region 16. The first implant is performed after the oxide etch and produces a P+ region 48 just below the N+ source region 18A. The implant 48 reduces the sheet resistance of the P-body 16A below the N+ source region 18A so as to completely avoid triggering bipolar transistor action during a collapse. The second P++ implant 26 is performed after etching the epitaxial layer 14 to form the trench 19A. The implant is used to increase the doping concentration of the source contact 28A at the interface of the P-body region 16A, thereby improving the contact between the source metal layer 28A and the P-body 16A. In the absence of the N+ buffer layer 17, the location of the collapse is fixed between the implanted region 48 and the N+ contact 23 or 23A, rather than just below the source contact implant region 26.
如同所討論的,該等P+/P++植入26、48係用以將該電晶體之電崩潰固定至該PN接面。該崩潰可經設計而發生在該 源極-主體接點下方之PN接面處或在該源極-主體接點與相距該源極接點若干橫向距離之汲極插塞23、23A之間。於該源極-主體接點26與該汲極插塞23A間發生之崩潰的第二情況係以數值模擬來確認。該模擬顯示該電晶體之斷面中於崩潰處的碰撞電離分佈。產生少數載子之最高速率係分佈在該源極-主體接點26之旁邊的P-主體16與該橫向擴散金屬氧化物半導體電晶體之汲極插塞23之間。此等具體實施例之主要影響在於出現於(例如)該電晶體關閉時之該等熱載子係遠離該閘極堆疊31而產生,進而改善該閘極氧化物36之可靠性。As discussed, the P+/P++ implants 26, 48 are used to secure the electrical breakdown of the transistor to the PN junction. The crash can be designed to occur in the The PN junction below the source-body junction or between the source-body junction and the drain plugs 23, 23A at a plurality of lateral distances from the source contact. The second case of collapse between the source-body contact 26 and the drain plug 23A was confirmed by numerical simulation. The simulation shows the impact ionization distribution at the collapse in the cross section of the transistor. The highest rate at which minority carriers are generated is distributed between the P-body 16 beside the source-body junction 26 and the drain plug 23 of the laterally diffused metal oxide semiconductor transistor. The primary effect of these embodiments is that the thermal carriers are generated away from the gate stack 31, for example, when the transistor is turned off, thereby improving the reliability of the gate oxide 36.
於一另一替代性具體實施例中,該崩潰位置係固定於圖13之P-緩衝區域21A或圖11及12之p-緩衝區域21與該汲極插塞23A之間,其中該汲極插塞結構23A係與摻雜多晶矽填充溝渠46相鄰並由源自摻雜多晶矽填充溝渠46內之摻雜物形成,如同圖12與13中顯示。此主要係由該PN接面處之摻雜濃度量來調整;若該濃度於該接面兩側均很高,則該崩潰電壓便很低。於此具體實施例中,該P-緩衝區域21A內之摻雜物濃度係增加至超過如上所討論之電荷耦合設計準則的提議最佳值,進而在該P-緩衝21A與該等汲極-插塞區域23、23A間之介面處產生一較低的崩潰。刻意違反上所討論之電荷耦合設計準則以便能將該崩潰電壓固定於此位置。該P-緩衝層21濃度係恰增至固定該崩潰所需之最大濃度。於一項具體實施例中,該濃度係增加約30至50%。於圖13之具體實施例中並無使用任何N-緩衝層,因為該N- 緩衝之濃度增加會將該崩潰電壓固定在該P+接點植入26之下。該N-緩衝於圖13之具體實施例中無須達到如上所述。In another alternative embodiment, the collapse location is fixed between the P-buffer region 21A of FIG. 13 or the p-buffer region 21 of FIGS. 11 and 12 and the drain plug 23A, wherein the collapse The plug structure 23A is adjacent to the doped polysilicon fill trench 46 and is formed of dopants from the doped polysilicon fill trench 46, as shown in Figures 12 and 13. This is mainly determined by the amount of doping concentration at the PN junction; if the concentration is high on both sides of the junction, the breakdown voltage is low. In this embodiment, the dopant concentration in the P-buffer region 21A is increased beyond the proposed optimal value of the charge-coupling design criteria as discussed above, and in the P-buffer 21A and the drain- A lower collapse occurs at the interface between the plug regions 23, 23A. Deliberately violate the charge-coupling design guidelines discussed above to be able to fix the breakdown voltage at this location. The concentration of the P-buffer layer 21 is just increased to the maximum concentration required to fix the collapse. In a specific embodiment, the concentration is increased by about 30 to 50%. No N-buffer layer is used in the specific embodiment of Figure 13, because the N- An increase in the concentration of the buffer will fix the breakdown voltage below the P+ contact implant 26. The N-buffering does not need to be as described above in the specific embodiment of FIG.
圖14係一巨集單元(macro-cell)裝置100(在本文中有時稱為"準橫向之橫向擴散金屬氧化物半導體裝置")之部分斷面圖,其包含複數個並聯耦合之橫向擴散金屬氧化物半導體電晶體裝置(如上文中結合圖11、12或13所說明者)。熟悉本技術人士將瞭解可運用圖1至5之橫向擴散金屬氧化物半導體電晶體形成相似的巨集單元裝置。此等巨集單元裝置之各種連接與組態係說明於共同待審且一般讓渡之Korec等人的美國專利申請案第11/254,482號中,該案之全部係以引用方式併入本文。儘管在裝置100中僅顯示兩個此類橫向擴散金屬氧化物半導體電晶體10D、10E或10F,然而應瞭解可並聯電耦合數百個此類裝置來形成一單一功能巨集單元裝置100。可由形成於該等裝置之上的匯流排結構(未顯示)產生此等單元之群組的連接。於一項具體實施例中,每一巨集單元裝置100包括介於約50至200(且較佳地約100)個橫向擴散金屬氧化物半導體電晶體10D,每一橫向擴散金屬氧化物半導體電晶體10D具有約2 μm或更小的間距。如同於該'482申請案中所說明以及於下文中更完整之說明,一示範性晶片級或近乎晶片級功率橫向擴散金屬氧化物半導體裝置包括數個巨集單元裝置100,其透過該匯流排結構而耦合在一起以如一單一功率橫向擴散金屬氧化物半導體裝置般地操作。Figure 14 is a partial cross-sectional view of a macro-cell device 100 (sometimes referred to herein as a "quasi-lateral laterally diffused metal-oxide-semiconductor device") that includes a plurality of parallel diffusions of lateral diffusion. Metal oxide semiconductor transistor device (as described above in connection with Figures 11, 12 or 13). Those skilled in the art will appreciate that similar lateral unit arrangements can be formed using the laterally diffused metal oxide semiconductor transistors of Figures 1 through 5. The various connections and configurations of such macrocell devices are described in co-pending and commonly assigned U.S. Patent Application Serial No. 11/254,482, the entire disclosure of which is incorporated herein by reference. Although only two such laterally diffused metal oxide semiconductor transistors 10D, 10E or 10F are shown in device 100, it should be understood that hundreds of such devices can be electrically coupled in parallel to form a single functional macrocell device 100. The connections of groups of such units may be generated by busbar structures (not shown) formed on the devices. In one embodiment, each macrocell device 100 includes between about 50 and 200 (and preferably about 100) laterally diffused metal oxide semiconductor transistors 10D, each laterally diffused metal oxide semiconductor The crystal 10D has a pitch of about 2 μm or less. An exemplary wafer level or near wafer level power laterally diffused metal oxide semiconductor device includes a plurality of macro cell devices 100 through which the busbars are as described in the '482 application and described more fully below. The structures are coupled together to operate as a single power laterally diffused metal oxide semiconductor device.
圖14中顯示之個別橫向擴散金屬氧化物半導體電晶體之 細節係結合圖11至13而說明於上文。如同結合圖11至13所說明且如同圖14中顯示,該源極接點電極28係佈置於該裝置100之頂表面上。然而,不同於圖11至13之具體實施例,包含上文中結合源極電極28所說明之導電材料的汲極電極104亦位於該裝置100之頂側,而非將該汲極電極置於該裝置100之底表面上(即,於該基板12之底表面上所形成之汲極電極11(圖11至13))。此特徵使一功率MOSFET之設計能具有高電流密度,如同該'482申請案中所說明。該汲極電極104係以於該磊晶層14之頂表面上所形成之絕緣層108與該源極電極28隔離。汲極電極104係經由高密度植入區域102而耦合至該基板12。電流從植入區域23先穿透基板12,然後橫向流至導電區域102中(該導電區域102集合來自多單元群組之電流),隨後並垂直流至該汲極電極104中。可以形成植入區域23之同一程序來形成該植入區域102,然而在該程序之後恰於該磊晶層14之上表面15之下並恰達該磊晶層14之上表面15接著進行一額外接點植入以確保高摻雜濃度,因而能與汲極電極104有良好的電接觸。Individual laterally diffused metal oxide semiconductor transistors shown in FIG. The details are described above in connection with Figures 11 to 13. The source contact electrode 28 is disposed on the top surface of the device 100 as explained in connection with FIGS. 11 through 13 and as shown in FIG. However, unlike the specific embodiment of Figures 11 through 13, the gate electrode 104 comprising the conductive material described above in connection with the source electrode 28 is also located on the top side of the device 100, rather than placing the gate electrode The bottom surface of the device 100 (i.e., the drain electrode 11 (Figs. 11 to 13) formed on the bottom surface of the substrate 12). This feature enables a power MOSFET design to have a high current density, as illustrated in the '482 application. The drain electrode 104 is isolated from the source electrode 28 by an insulating layer 108 formed on the top surface of the epitaxial layer 14. The drain electrode 104 is coupled to the substrate 12 via a high density implant region 102. Current first penetrates the substrate 12 from the implanted region 23 and then flows laterally into the conductive region 102 (which concentrates the current from the multi-cell group) and then flows vertically into the drain electrode 104. The same procedure can be used to form the implant region 23 to form the implant region 102, however, after the procedure, just below the upper surface 15 of the epitaxial layer 14 and just above the epitaxial layer 14 surface 15 is followed by a Additional contacts are implanted to ensure a high doping concentration and thus good electrical contact with the drain electrode 104.
圖15說明圖15之巨集單元裝置的替代性具體實施例。圖14之裝置100A包括一P-摻雜基板12A而非一N-摻雜基板12。上述之電晶體10D、10E或10F係形成於一埋置層106上,該埋置層106係一形成於該磊晶層14A中的高度摻雜N+層。該埋置層106將來自該等電晶體之電流橫向承載至植入插塞102,該植入插塞102將該電流提供至該汲極電極 104。該埋置層106提供該等橫向擴散金屬氧化物半導體電晶體與該基板12A的電絕緣,並使若干獨立橫向擴散金屬氧化物半導體(或其他裝置)能夠整合於一共同基板12A上。例如,裝置100A可以多重獨立整合功率切換器形成一功率管理IC。儘管於圖15中未顯示,然而該橫向擴散金屬氧化物半導體裝置之間距亦可藉由使該源極接點開口自對準該閘極結構而減小,如同結合圖13之橫向擴散金屬氧化物半導體裝置10F所說明。Figure 15 illustrates an alternative embodiment of the macrocell device of Figure 15. The device 100A of FIG. 14 includes a P-doped substrate 12A instead of an N-doped substrate 12. The above-mentioned transistor 10D, 10E or 10F is formed on a buried layer 106 which is a highly doped N+ layer formed in the epitaxial layer 14A. The buried layer 106 laterally carries current from the transistors to the implant plug 102, which provides the current to the drain electrode 104. The buried layer 106 provides electrical isolation of the laterally diffused metal oxide semiconductor transistors from the substrate 12A and enables a plurality of independent laterally diffused metal oxide semiconductors (or other devices) to be integrated on a common substrate 12A. For example, device 100A can form a power management IC by multiple independent integrated power switches. Although not shown in FIG. 15, the lateral diffusion metal oxide semiconductor device spacing can also be reduced by self-aligning the source contact opening to the gate structure, as in the lateral diffusion metal oxidation in conjunction with FIG. The semiconductor device 10F is described.
如同上文中所提及,於若干具體實施例中,所提供之經改善功率橫向擴散金屬氧化物半導體裝置具有一n-通道電晶體,其於一低電阻N-基板上形成。該裝置會藉由降低對該基板之電阻影響而展現低導通電阻(Rds-on )以及藉由使該等閘極電極與汲極電極間之靜電耦合降至最低而展現低Cgd電容。可減小該增強汲極漂移區域之長度,並使裝置能產生較小間距卻仍具有與先前技術裝置相同的崩潰電壓。如此,接著使裝置密度與電流能力能夠改善。As mentioned above, in several embodiments, the improved power laterally diffused metal oxide semiconductor device is provided with an n-channel transistor formed on a low resistance N-substrate. The device exhibits a low on-resistance (R ds-on ) by reducing the resistance of the substrate and exhibits a low Cgd capacitance by minimizing electrostatic coupling between the gate electrodes and the drain electrodes. The length of the enhanced drain drift region can be reduced and the device can produce a smaller pitch while still having the same collapse voltage as prior art devices. As such, the device density and current capability can then be improved.
於若干具體實施例中,選擇該摻雜分佈並組態汲極連接以最佳化該崩潰位置。可將該裝置組態成在對該P-主體層之P+接點附近之PN接面的預定義位置發生崩潰。碰撞電離速率最高之區域可從該P+接點朝該基板垂直擴散或朝該汲極插塞區域橫向擴展以使該崩潰遠離該閘極堆疊而固定並降低觸發該雙極電晶體的危險。該崩潰位置亦可位於一P-緩衝層與該埋置汲極接點間。該摻雜結構會控制該高碰撞電離速率以垂直或水平方式來擴展。使該崩潰位置最佳 化有助於避免如本文中所說明之裝置崩潰。In several embodiments, the doping profile is selected and a drain connection is configured to optimize the collapse location. The device can be configured to collapse at a predefined location of the PN junction near the P+ junction of the P-body layer. The region of highest impact ionization rate may extend vertically from the P+ junction toward the substrate or laterally toward the drain plug region to cause the collapse to be fixed away from the gate stack and reduce the risk of triggering the bipolar transistor. The collapse location can also be between a P-buffer layer and the buried drain contact. The doped structure controls the high impact ionization rate to expand in a vertical or horizontal manner. Make the crash location the best This helps to avoid device crashes as explained in this article.
以圖11作為一說明性範例,本文中所說明之功率橫向擴散金屬氧化物半導體反映一種設計一LDD區域20的創新方法,該LDD區域20基於該電壓支持LDD區域20(圖11)與一相反極性摻雜區域(例如,圖11之P-緩衝層21)之電荷平衡與該源極電極28與該汲極延伸區域20間之緊密電容電荷控制電極耦合(即,該源極電極28將在該延伸區域20中誘發電場,因為其上重疊用作隔離的介電質)。該相反極性與電極區域之組合會在漂移層20內側維持一高電場,從而改善電壓額定並使其摻雜能增加並使其長度縮短,進而使該電晶體單元與其Rds,on大小減小。Using FIG. 11 as an illustrative example, the power laterally diffused metal oxide semiconductor described herein reflects an innovative method of designing an LDD region 20 that supports the LDD region 20 (FIG. 11) based on the voltage. The charge balance of the polar doped region (eg, P-buffer layer 21 of FIG. 11) is coupled to the tight capacitance charge control electrode between the source electrode 28 and the drain extension region 20 (ie, the source electrode 28 will be An electric field is induced in the extended region 20 because it overlaps as a dielectric for isolation). The combination of the opposite polarity and the electrode region maintains a high electric field inside the drift layer 20, thereby improving the voltage rating and increasing its doping energy and shortening its length, thereby reducing the size of the transistor unit and its Rds,on.
一旦三區域(汲極延伸20、P-緩衝21與源極電極28)均近乎電荷平衡便能實現崩潰電壓與最小漂移層電阻的最完美設計。以上所述將在該汲極延伸區域20中之總淨摻雜與摻雜物分佈幾乎等於其下之相反極性摻雜區域(即,P-緩衝層21)中之淨摻雜與摻雜物分佈時發生。該頂源極電極28欲與該LDD區域20電荷平衡時,選擇介電層34之介電層厚度以使該LDD區域20內側具有電場,該電場大到足以改善崩潰但卻不大於LDD區域20中的臨限電場,如此將導致一較低的過早突崩潰。Once the three regions (the drain extension 20, the P-buffer 21 and the source electrode 28) are nearly charge balanced, the perfect design of the breakdown voltage and the minimum drift layer resistance can be achieved. The total net doping and dopant distribution in the drain extension region 20 is almost equal to the net doping and dopant in the opposite polarity doping region (ie, the P-buffer layer 21). Occurs when distributing. When the top source electrode 28 is to be charge-balanced with the LDD region 20, the dielectric layer thickness of the dielectric layer 34 is selected such that the LDD region 20 has an electric field inside, which is large enough to improve the collapse but not greater than the LDD region 20. The limited electric field in the middle will cause a lower premature burst.
一旦最佳化摻雜與氧化物厚度(如利用數值模擬之引導),在該LDD區域20中將維持一高電場,並導致崩潰電壓增加,因為該電壓係沿該LDD區域20之長度該電場之面積的積分。與傳統裝置不同,一額外好處在於可使用該 LDD層20之較高摻雜,因為該崩潰電壓並不受限於該LDD摻雜。因此,可使用該較高摻雜以在整個LDD層20中維持高電場。該電荷平衡LDD層20之電壓額定可僅藉由增加該LDD區域20之長度來增加,而與必須降低該摻雜以使該LDD區域之長度增加的傳統裝置不同。Once the doping and oxide thickness are optimized (as guided by numerical simulation), a high electric field will be maintained in the LDD region 20 and cause a breakdown voltage to increase because the voltage is along the length of the LDD region 20. The integral of the area. Unlike traditional devices, an added benefit is that it can be used The higher doping of the LDD layer 20 is because the breakdown voltage is not limited to the LDD doping. Therefore, this higher doping can be used to maintain a high electric field throughout the LDD layer 20. The voltage rating of the charge balancing LDD layer 20 can be increased only by increasing the length of the LDD region 20, as opposed to conventional devices that must reduce the doping to increase the length of the LDD region.
於某些具體實施例中,可藉由將該P-緩衝層21摻雜超過上述之最佳平衡而故意使該橫向擴散金屬氧化物半導體電晶體裝置中發生電荷的若干失衡。咸信此摻雜分佈依突崩潰處理能力之觀點應係有利的,因為其會用以將大部分崩潰電流侷限在該緩衝層21中,同時使其他層釋放該崩潰電流。此屬性之重要性在於將功率裝置設計成具有健全的突崩處理能力,因為該等功率裝置係用於電路中,而該等電路會因發生故障或啟動條件使裝置曝露於突崩潰。藉由將該電流侷限於該P-緩衝層21,將透過該P++層26來擷取該電流。此電流流動路徑產生最低電流電阻以減少發熱,並亦使電流免於在該源極之下流動,從而避免寄生雙極鎖存(開啟)。In some embodiments, several imbalances in charge can occur in the laterally diffused metal oxide semiconductor transistor device by doping the P-buffer layer 21 beyond the optimum balance described above. It is believed that this doping profile is advantageous in terms of the ability to handle the collapse, as it would be used to confine most of the breakdown current in the buffer layer 21 while allowing other layers to release the breakdown current. The importance of this property is that the power devices are designed to have robust sag handling capabilities because such power devices are used in circuits that expose the device to sudden collapse due to failure or starting conditions. By confining this current to the P-buffer layer 21, the current will be drawn through the P++ layer 26. This current flow path produces the lowest current resistance to reduce heat generation and also protects the current from flowing under the source, thereby avoiding parasitic bipolar latching (on).
儘管本發明已依據示範性具體實施例上加以說明,然而卻並未對其予以限定。而是,所附申請專利範圍應廣義地理解為包括本發明之其他變化與具體實施例,其可由熟悉本技術人士所製造而不脫離本發明之等效範疇與範圍。Although the present invention has been described in terms of exemplary embodiments, it is not limited thereto. Rather, the scope of the invention is to be construed as being limited by the scope of the invention.
10‧‧‧LDMOS/裝置10‧‧‧LDMOS/device
10A‧‧‧LDMOS/裝置10A‧‧‧LDMOS/device
10B‧‧‧LDMOS/裝置10B‧‧‧LDMOS/device
10C‧‧‧LDMOS/裝置10C‧‧‧LDMOS/device
10D‧‧‧LDMOS/裝置10D‧‧‧LDMOS/device
10E‧‧‧LDMOS/裝置10E‧‧‧LDMOS/device
10F‧‧‧LDMOS/裝置10F‧‧‧LDMOS/device
11‧‧‧汲極電極/背側金屬層11‧‧‧汲electrode/backside metal layer
12‧‧‧基板12‧‧‧Substrate
12A‧‧‧基板12A‧‧‧Substrate
14‧‧‧磊晶層14‧‧‧ epitaxial layer
14A‧‧‧磊晶層14A‧‧‧Elevation layer
15‧‧‧上表面/頂表面15‧‧‧Upper surface/top surface
16‧‧‧主體區域/P井16‧‧‧Main Area/P Well
16A‧‧‧主體區域16A‧‧‧Main Area
16B‧‧‧主體植入區域16B‧‧‧Subject area
17‧‧‧緩衝層17‧‧‧ Buffer layer
18‧‧‧源極(區域)/源極植入18‧‧‧Source (region) / source implant
18A‧‧‧N+源極區域18A‧‧‧N+ source area
19‧‧‧淺溝渠19‧‧‧Shallow Ditch
19A‧‧‧淺溝渠19A‧‧‧Shallow Ditch
20‧‧‧汲極區域20‧‧‧Bungee area
20A‧‧‧汲極延伸區域20A‧‧‧Bungee Extension Area
21‧‧‧P-緩衝層21‧‧‧P-buffer layer
21A‧‧‧P-緩衝區域21A‧‧‧P-buffer area
22‧‧‧汲極接點區域/汲極接點植入22‧‧‧汲 Contact area/dual contact implant
23‧‧‧汲極接點區域/N+摻雜區域/汲極插塞23‧‧‧汲 contact area/N+ doped area/bungee plug
23A‧‧‧汲極插塞23A‧‧‧汲pole plug
24‧‧‧插塞24‧‧‧ Plug
25‧‧‧深溝渠區域25‧‧‧Deep trench area
26‧‧‧主體接點區域/植入區域/P++層26‧‧‧Main contact area/implant area/P++ layer
28‧‧‧源極金屬層/電極28‧‧‧Source metal layer/electrode
28A‧‧‧源極金屬層/電極28A‧‧‧Source metal layer/electrode
29‧‧‧上表面29‧‧‧Upper surface
30‧‧‧多晶矽層30‧‧‧Polysilicon layer
31‧‧‧導電閘極/閘極堆疊31‧‧‧ Conductive gate/gate stack
32‧‧‧矽化物層32‧‧‧ Telluride layer
34‧‧‧絕緣層/氧化物層/介電層34‧‧‧Insulation/Oxide/Dielectric Layer
34A‧‧‧絕緣層34A‧‧‧Insulation
34B‧‧‧絕緣層34B‧‧‧Insulation
34C‧‧‧介電層34C‧‧‧ dielectric layer
35‧‧‧較厚部分35‧‧‧ thicker part
36‧‧‧閘極介電質/閘極氧化物36‧‧‧Gate dielectric/gate oxide
37‧‧‧較薄部分37‧‧‧ Thinner part
38‧‧‧第一緩衝區域38‧‧‧First buffer zone
38C‧‧‧緩衝層38C‧‧‧buffer layer
40‧‧‧緩衝層40‧‧‧buffer layer
46‧‧‧多晶矽插塞/多晶矽填充溝渠46‧‧‧Polysilicon plug/polysilicon filled trench
48‧‧‧植入/P+區域48‧‧‧ implanted/P+ area
100‧‧‧裝置100‧‧‧ device
100A‧‧‧裝置100A‧‧‧ device
102‧‧‧導電區域/植入區域/植入插塞102‧‧‧Conducting area/implantation area/implantation plug
104‧‧‧汲極電極104‧‧‧汲electrode
106‧‧‧埋置層106‧‧‧buried layer
108‧‧‧絕緣層108‧‧‧Insulation
該等附圖會說明本發明之較佳具體實施例,以及與本揭示案有關的其他資訊,其中: 圖1說明根據本發明之一橫向擴散金屬氧化物半導體電晶體;圖2說明本發明之一橫向擴散金屬氧化物半導體電晶體的一項具體實施例,其具有改善的場板效應;圖3說明本發明之一橫向擴散金屬氧化物半導體電晶體的一項具體實施例,其具有一用於抑制短通道效應之緩衝層;圖4說明圖3之一橫向擴散金屬氧化物半導體電晶體的一項具體實施例,其具有一用於改善該改善電晶體之崩潰特性的第二緩衝層;圖5說明一與一半導體基板之側邊緣相鄰的區域,其上形成該改善的橫向擴散金屬氧化物半導體電晶體;圖6至10顯示藉由數值模擬所獲關於該改善之功率橫向擴散金屬氧化物半導體裝置的電特性;圖11說明根據本發明之一替代性具體實施例之一橫向擴散金屬氧化物半導體電晶體;圖12說明圖11之橫向擴散金屬氧化物半導體電晶體的替代性具體實施例;圖13說明圖12之橫向擴散金屬氧化物半導體電晶體的替代性具體實施例;圖14說明包括複數個橫向擴散金屬氧化物半導體電晶體並具有朝上定向之源極與汲極電極之半導體裝置;以及圖15說明圖14之裝置組態的替代性具體實施例。The drawings will illustrate preferred embodiments of the invention, as well as additional information related to the present disclosure, in which: 1 illustrates a laterally diffused metal oxide semiconductor transistor in accordance with the present invention; and FIG. 2 illustrates a specific embodiment of a laterally diffused metal oxide semiconductor transistor of the present invention having improved field plate effect; FIG. A specific embodiment of a laterally diffused metal oxide semiconductor transistor of the present invention having a buffer layer for suppressing short channel effects; and FIG. 4 illustrates a lateral diffusion metal oxide semiconductor transistor of FIG. a specific embodiment having a second buffer layer for improving the collapse characteristics of the improved transistor; FIG. 5 illustrates a region adjacent to a side edge of a semiconductor substrate on which the improved laterally diffused metal oxide is formed Semiconductor transistor; Figures 6 through 10 show electrical characteristics of the power laterally diffused metal oxide semiconductor device obtained by numerical simulation; Figure 11 illustrates lateral diffusion metal oxide in accordance with an alternative embodiment of the present invention Semiconductor semiconductor transistor; FIG. 12 illustrates an alternative embodiment of the laterally diffused metal oxide semiconductor transistor of FIG. 11; FIG. An alternative embodiment of the laterally diffused metal oxide semiconductor transistor of FIG. 12; FIG. 14 illustrates a semiconductor device including a plurality of laterally diffused metal oxide semiconductor transistors having source and drain electrodes oriented upward; 15 illustrates an alternative embodiment of the device configuration of FIG.
10D‧‧‧LDMOS/裝置10D‧‧‧LDMOS/device
11‧‧‧汲極電極/背側金屬層11‧‧‧汲electrode/backside metal layer
12‧‧‧基板12‧‧‧Substrate
14‧‧‧磊晶層14‧‧‧ epitaxial layer
15‧‧‧上表面/頂表面15‧‧‧Upper surface/top surface
16‧‧‧主體區域/P井16‧‧‧Main Area/P Well
17‧‧‧緩衝層17‧‧‧ Buffer layer
18‧‧‧源極(區域)/源極植入18‧‧‧Source (region) / source implant
19‧‧‧淺溝渠19‧‧‧Shallow Ditch
20‧‧‧汲極區域20‧‧‧Bungee area
21‧‧‧p-緩衝層21‧‧‧p-buffer layer
23‧‧‧汲極接點區域/N+摻雜區域/汲極插塞23‧‧‧汲 contact area/N+ doped area/bungee plug
26‧‧‧主體接點區域/植入區域/P++層26‧‧‧Main contact area/implant area/P++ layer
28‧‧‧源極金屬層/電極28‧‧‧Source metal layer/electrode
29‧‧‧上表面29‧‧‧Upper surface
30‧‧‧多晶矽層30‧‧‧Polysilicon layer
31‧‧‧導電閘極/閘極堆疊31‧‧‧ Conductive gate/gate stack
32‧‧‧矽化物層32‧‧‧ Telluride layer
34‧‧‧絕緣層/氧化物層/介電層34‧‧‧Insulation/Oxide/Dielectric Layer
36‧‧‧閘極介電質/閘極氧化物36‧‧‧Gate dielectric/gate oxide
Claims (20)
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US11/676,613 US7589378B2 (en) | 2005-07-13 | 2007-02-20 | Power LDMOS transistor |
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TW200836342A TW200836342A (en) | 2008-09-01 |
TWI470796B true TWI470796B (en) | 2015-01-21 |
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TW96148715A TWI470796B (en) | 2007-02-20 | 2007-12-19 | Power ldmos transistor |
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TW (1) | TWI470796B (en) |
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JP5487852B2 (en) * | 2008-09-30 | 2014-05-14 | サンケン電気株式会社 | Semiconductor device |
US8916955B2 (en) | 2012-10-17 | 2014-12-23 | Taiwan Semiconductor Manufacturing Co., Ltd. | Nearly buffer zone free layout methodology |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6462378B1 (en) * | 1999-01-15 | 2002-10-08 | Fairchild Korea Semiconductor, Ltd. | Power MOSFET with decreased body resistance under source region |
US6600182B2 (en) * | 2001-09-26 | 2003-07-29 | Vladimir Rumennik | High current field-effect transistor |
US6768167B2 (en) * | 2002-05-21 | 2004-07-27 | Fuji Electric Co., Ltd. | MIS semiconductor device and the manufacturing method thereof |
US6989568B2 (en) * | 1999-12-27 | 2006-01-24 | Kabushiki Kaisha Toshiba | Lateral high-breakdown-voltage transistor having drain contact region |
-
2007
- 2007-12-19 TW TW96148715A patent/TWI470796B/en active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6462378B1 (en) * | 1999-01-15 | 2002-10-08 | Fairchild Korea Semiconductor, Ltd. | Power MOSFET with decreased body resistance under source region |
US6989568B2 (en) * | 1999-12-27 | 2006-01-24 | Kabushiki Kaisha Toshiba | Lateral high-breakdown-voltage transistor having drain contact region |
US6600182B2 (en) * | 2001-09-26 | 2003-07-29 | Vladimir Rumennik | High current field-effect transistor |
US6768167B2 (en) * | 2002-05-21 | 2004-07-27 | Fuji Electric Co., Ltd. | MIS semiconductor device and the manufacturing method thereof |
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