TWI724834B - Semiconductor device having floating conductive layer - Google Patents
Semiconductor device having floating conductive layer Download PDFInfo
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Abstract
Description
本發明是有關於一種半導體裝置,且特別是有關於一種具有浮置導體層的半導體裝置。The present invention relates to a semiconductor device, and more particularly to a semiconductor device having a floating conductor layer.
超高壓(ultra-high voltage, ultra-HV)半導體裝置廣泛用於顯示元件、可攜式元件與其他多元應用。超高壓半導體裝置所追求的目標包括具有高崩潰電壓(breakdown voltage)、低特徵導通電阻(specific on-resistance,Ron)並兼顧在室溫與高溫環境下的高可靠性。Ultra-high voltage (ultra-HV) semiconductor devices are widely used in display components, portable components and other diverse applications. The goals pursued by ultra-high voltage semiconductor devices include high breakdown voltage (breakdown voltage), low characteristic on-resistance (Ron), and high reliability in both room temperature and high temperature environments.
然而,隨著超高壓半導體裝置的應用面擴大,尋求更高的崩潰電壓已成為目前的研究重點。However, as the application of ultra-high voltage semiconductor devices expands, seeking a higher breakdown voltage has become the current research focus.
本發明提供一種具有浮置導體層的半導體裝置,能通過降低特徵導通電阻(Ron)提高崩潰電壓達500V以上。The present invention provides a semiconductor device with a floating conductor layer, which can increase the breakdown voltage to more than 500V by reducing the characteristic on-resistance (Ron).
本發明的半導體裝置,包括具有第一導電型的基板、具有第二導電型的高壓井、具有第一導電型的源極井、具有第二導電型的汲極井、隔離層、閘極層、源極區、汲極區與至少一浮置導體層。高壓井形成於基板中,源極井形成於高壓井一側的基底中,汲極井形成於高壓井中,隔離層形成於源極井與汲極井之間的高壓井上方,閘極層形成於基板上方並自源極井之邊緣部分上方連續延伸至隔離層的邊緣部分上方,源極區形成於閘極層旁的源極井中,浮置導體層則是形成於隔離層上方。所述浮置導體層與汲極區之間的距離小於浮置導體層與源極區之間的距離。The semiconductor device of the present invention includes a substrate having a first conductivity type, a high-voltage well having a second conductivity type, a source well having a first conductivity type, a drain well having a second conductivity type, an isolation layer, and a gate layer , The source region, the drain region and at least one floating conductor layer. The high-pressure well is formed in the substrate, the source well is formed in the base on one side of the high-pressure well, the drain well is formed in the high-pressure well, the isolation layer is formed above the high-pressure well between the source well and the drain well, and the gate layer is formed Above the substrate and continuously extending from the edge portion of the source well to the edge portion of the isolation layer, the source region is formed in the source well beside the gate layer, and the floating conductor layer is formed above the isolation layer. The distance between the floating conductor layer and the drain region is smaller than the distance between the floating conductor layer and the source region.
為讓本發明的上述特徵和優點能更明顯易懂,下文特舉實施例,並配合所附圖式作詳細說明如下。In order to make the above-mentioned features and advantages of the present invention more comprehensible, the following specific embodiments are described in detail in conjunction with the accompanying drawings.
以下內容提供許多不同的實施方式或實施例,用於實施本發明的不同特徵。而且,這些實施例僅為示範例,並不用來限制本發明的範圍與應用。再者,為了清楚起見,各區域或結構元件的相對尺寸(如長度、厚度、間距等)及相對位置可能縮小或放大。另外,在各圖式中使用相似或相同的元件符號表示相似或相同元件或特徵。The following content provides many different implementations or examples for implementing different features of the present invention. Moreover, these embodiments are only exemplary, and are not used to limit the scope and application of the present invention. Furthermore, for the sake of clarity, the relative size (such as length, thickness, spacing, etc.) and relative position of each region or structural element may be reduced or enlarged. In addition, similar or identical element symbols are used in the various drawings to indicate similar or identical elements or features.
圖1是依照本發明的一實施例的一種半導體裝置的俯視示意圖,圖2是圖1的II-II’線段的半導體裝置的剖面示意圖。FIG. 1 is a schematic top view of a semiconductor device according to an embodiment of the present invention, and FIG. 2 is a schematic cross-sectional view of the semiconductor device along the line II-II' in FIG. 1.
請參照圖1與圖2,本實施例的半導體裝置10包括具有第一導電型的基板100、具有第二導電型的高壓井102、具有第一導電型的源極井104、具有第二導電型的汲極井106、隔離層108、閘極層110、源極區112、汲極區114與至少一浮置導體層116。在一實施例中,上述第一導電型為P型,上述第二導電型為N型。在另一實施例中,上述第一導電型為N型,上述第二導電型為P型。基板100為半導體基板,例如由矽塊材、磊晶層(epitaxial layer)或絕緣層上矽(silicon-on-insulator,SOI)材料形成。在本實施例中,半導體裝置10可為橫向擴散金氧半場效電晶體(Lateral Diffused MOSFET)裝置,並且可應用於混合模式(mix-mode)電路設計或模擬電路設計,例如:LED照明、省電燈具、安定器(ballast)、馬達驅動器(motor driver)等。高壓井102形成於基板100中,源極井104則形成於高壓井102一側的基底100中,汲極井106形成於高壓井102中。在一實施例中,源極井104與高壓井102互相鄰接。上述源極區112則形成於閘極層110旁的源極井104中,且源極區104包括有第一導電型的第一重摻雜區118與具有第二導電型的第二重摻雜區120,所述第二重摻雜區120形成在第一重摻雜區118與閘極層110之間。1 and 2, the
所述隔離層108形成於源極井104與汲極井106之間的高壓井102上方,而且在主動區或氧化界定(OD)區以外設置有場氧化(field oxide,FOX)層122之類的隔離結構,且這些隔離結構與隔離層108可以同一道熱氧化步驟製得,然而本發明並不限於此,上述隔離結構也可改為局部矽氧化層(LOCOS)或淺溝渠隔離結構(STI)。在一實施例中,隔離層108與汲極井106部分重疊,並與源極井104分隔。The
所述閘極層110是形成於基板100上方並自源極井104之邊緣部分104a上方連續延伸至隔離層108的邊緣部分108a上方,且於閘極層110與基板100之間一般設置有閘氧化層(未繪示),在閘極層110的側壁可形成間隙壁(未繪示)。閘極層110的材料可為多晶矽或其他適合的導體材料。The
所述浮置導體層116則是形成於隔離層108上方,且浮置導體層116與汲極區114之間的距離s1小於浮置導體層116與源極區112之間的距離s2;也就是說,浮置導體層116的位置較接近汲極區114,並遠離源極井104。由於隔離層108上方設置了電性上浮置的浮置導體層116,所以在汲極區114施加超高壓(如500V以上),隔離層108下方的電場分布將如圖4所示,藉由浮置導體層116的存在而保持一小段固定的電場再往源極區112增加,可避免電壓突升的情形發生並降低Ron,使崩潰電壓進一步增加。相較下,沒有設置浮置導體層的電場分布明顯會有突升區400。在一實施例中,浮置導體層116與汲極區114之間的距離s1可保持在1µm以上,在一實施例中是在4 µm以上,在另一實施例中是在8µm以上,並搭配寬w1度約4µm的浮置導體層116,即可使崩潰電壓達到500V以上。在一實施例中,浮置導體層116的寬度w1是隔離層108的寬度w2 (請見圖1)的0.025倍~0.8倍。在一實施例中,浮置導體層116的厚度t1是隔離層108的厚度t2的0.2倍~0.3倍,例如0.22倍~0.3倍。浮置導體層116的材料包括多晶矽或金屬(例如鋁);若是多晶矽的話,浮置導體層116可與閘極層110同時形成,因此能避免增加額外的步驟。然而,本發明並不限於此。The
在圖2中,半導體裝置10還可包括一飄移區124,形成於隔離層108下方的高壓井102中。在本實施例中,飄移區124包括具有第一導電型的頂(top)區126與具有第二導電型的梯度(grade)區128,梯度區128形成於隔離層108與頂區126之間。在一實施例中,梯度區128可延伸出隔離層108並與閘極層110相接。而且,飄移區124可位於浮置導體層116的正下方或與浮置導體層116部分重疊。In FIG. 2, the
圖3是依照本發明的另一實施例的一種半導體裝置的剖面示意圖,其中使用上一實施例的元件符號來表示相同或類似的構件,且相同的構件的說明可參照上一實施例的相關內容,於此不再贅述。3 is a schematic cross-sectional view of a semiconductor device according to another embodiment of the present invention, in which the component symbols of the previous embodiment are used to denote the same or similar components, and the description of the same components can refer to the related descriptions of the previous embodiment The content will not be repeated here.
在圖3中,形成於隔離層108上方的是兩個浮置導體層300a與300b,其中浮置導體層300b與汲極區114之間的距離s1小於浮置導體層300a與源極區112之間的距離s2,且距離s1可保持在1 µm以上,例如在8µm以上。也就是說,將浮置導體層300a與300b視為一個整體,所以即使浮置導體層300a與300b之間互不耦接,整體來看也是較接近汲極區114而遠離源極井104。雖然圖3顯示的兩個浮置導體層300a與300b,然而本發明並不限於此,浮置導體層的數量也可大於2,如3個、4個…等。而浮置導體層300a與300b的寬度w3則可為隔離層108的寬度w2的0.025倍~0.37倍。In FIG. 3, formed above the
以下列舉數個實驗,更具體地驗證本發明的半導體裝置的功效。然而,在不逾越本發明範疇的情況下,可適當地改變所用材料、數量及尺寸比率、參數以及量測方式等等。因此,不應根據下文所述的實驗對本發明作出限制性的解釋。Several experiments are listed below to more specifically verify the efficacy of the semiconductor device of the present invention. However, without going beyond the scope of the present invention, the materials used, quantity and size ratio, parameters, measurement methods, etc. can be appropriately changed. Therefore, the present invention should not be interpreted restrictively based on the experiments described below.
〈實驗例1〉<Experimental example 1>
製作如圖2所示的半導體裝置,其中N型高壓井(102)的標準劑量(STD)是3.5E12/cm 2、P型頂區(126)的標準劑量(STD)是8E12/cm 2,且固定浮置導體層與汲極區之間的距離(s1)為8µm。然後,多晶矽的浮置導體層的寬度分別為4µm、6µm與8µm,測其在改變N型高壓井的劑量比例的情況下,崩潰電壓(BVD)的變化曲線,結果顯示於圖5。 Fabricate the semiconductor device as shown in Figure 2, where the standard dose (STD) of the N-type high pressure well (102) is 3.5E12/cm 2 , and the standard dose (STD) of the P-type top zone (126) is 8E12/cm 2 , And the distance (s1) between the fixed floating conductor layer and the drain region is 8 µm. Then, the widths of the floating conductor layer of polysilicon were 4μm, 6μm and 8μm, and the breakdown voltage (BVD) curve was measured when the dose ratio of the N-type high-voltage well was changed. The results are shown in Fig. 5.
〈實驗例2〉<Experimental example 2>
製作如圖2所示的半導體裝置,其中多晶矽浮置導體層的厚度約1300Å、氧化矽隔離層的厚度約6000Å、N型高壓井(102)的標準劑量(STD)是3.5E12/cm 2、P型頂區(126)的標準劑量(STD)是8E12/cm 2,且固定浮置導體層與汲極區之間的距離(s1)為8µm。然後,多晶矽的浮置導體層的寬度分別為4µm、6µm與8µm,測其在改變P型頂區的劑量比例的情況下,崩潰電壓的變化曲線,結果顯示於圖6。 Fabricate the semiconductor device shown in Figure 2, where the thickness of the polysilicon floating conductor layer is about 1300 Å, the thickness of the silicon oxide isolation layer is about 6000 Å, and the standard dose (STD) of the N-type high pressure well (102) is 3.5E12/cm 2 , The standard dose (STD) of the P-type top region (126) is 8E12/cm 2 , and the distance (s1) between the fixed floating conductor layer and the drain region is 8 μm. Then, the widths of the floating conductor layer of polysilicon were 4μm, 6μm and 8μm, and the change curve of breakdown voltage was measured when the dose ratio of the P-type top region was changed.
〈比較例1〉<Comparative Example 1>
製作如圖2所示的半導體裝置,但沒有浮置導體層,其餘條件與實驗例1一樣,並測其在改變N型高壓井的劑量比例的情況下,崩潰電壓的變化曲線,結果顯示於圖5。The semiconductor device as shown in Figure 2 was fabricated, but there was no floating conductor layer, and the remaining conditions were the same as in Experimental Example 1. The change curve of the breakdown voltage was measured when the dose ratio of the N-type high-voltage well was changed. The results are shown in Figure 5.
〈比較例2〉<Comparative Example 2>
製作如圖2所示的半導體裝置,但沒有浮置導體層,其餘條件與實驗例2一樣,並測其在改變P型頂區的劑量比例的情況下,崩潰電壓的變化曲線,結果顯示於圖6。The semiconductor device as shown in Figure 2 was fabricated, but there was no floating conductor layer, and the remaining conditions were the same as in Experimental Example 2. The change curve of the breakdown voltage was measured when the dose ratio of the P-type top region was changed. The results are shown in Figure 6.
從圖5可得到,具有浮置導體層的實驗例1的崩潰電壓隨N型高壓井的劑量增加而增加,代表n的電荷大於p的電荷(Qn>Qp)可增加崩潰電壓;從圖6可得到,具有浮置導體層的實驗例2的崩潰電壓隨P型頂區的劑量減少而增加,也代表Qn>Qp可增加崩潰電壓。相較之下,無浮置導體層的比較例1~2則沒有出現上述趨勢。It can be obtained from Fig. 5 that the breakdown voltage of Experimental Example 1 with a floating conductor layer increases with the increase of the dose of the N-type high voltage well, which means that the charge of n is greater than the charge of p (Qn>Qp) can increase the breakdown voltage; from Fig. 6 It can be obtained that the breakdown voltage of Experimental Example 2 with a floating conductor layer increases as the dose of the P-type top region decreases, which also means that Qn>Qp can increase the breakdown voltage. In contrast, Comparative Examples 1 to 2 with no floating conductor layer did not show the above trend.
〈Ron分析〉<Ron Analysis>
取得實驗例1~2(浮置導體層寬度為4µm)中崩潰電壓達500V以上的N型高壓井的劑量+7%以及P型頂區的劑量-9%的Ron,連同沒有浮置導體層且N型高壓井和P型頂區的劑量均為標準值的Ron一起記載於圖7。從圖7中三次測得的Ron可得到,有浮置導體層的情況下,若是N型高壓井的劑量為+7%的標準劑量或者P型頂區的劑量為-9%的標準劑量,都能改善Ron達5%以上。因此,按照推論,同時調整N型高壓井的劑量與P型頂區的劑量也能使Ron進一步降低。Obtain the dose of N-type high-voltage well +7% and the dose of P-type top region -9% for the N-type high voltage well with a breakdown voltage of more than 500V in Experimental Examples 1~2 (the width of the floating conductor layer is 4µm), and there is no floating conductor layer. Ron, where the doses of the N-type high pressure well and the P-type top zone are both standard values, are shown in Fig. 7. It can be obtained from the Ron measured three times in Fig. 7 that if there is a floating conductor layer, if the dose of the N-type high pressure well is +7% of the standard dose or the dose of the P-type top zone is -9% of the standard dose, Both can improve Ron by more than 5%. Therefore, according to the inference, adjusting the dose of the N-type high-pressure well and the dose of the P-type top zone at the same time can also further reduce Ron.
綜上所述,本發明在隔離層上方設置了浮置導體層,所以能在汲極區施加超高壓(如500V以上)時,使電場分布因為浮置導體層的存在而保持一段固定的電場,再往源極區增加,因此能避免電壓突升的情形發生並降低Ron,進而增加崩潰電壓,有利於超高壓元件的應用。In summary, the present invention provides a floating conductor layer above the isolation layer, so that when an ultra-high voltage (such as 500V or more) is applied to the drain region, the electric field distribution can maintain a fixed electric field due to the existence of the floating conductor layer. , And then increase to the source region, so it can avoid the voltage surge and reduce Ron, and then increase the breakdown voltage, which is beneficial to the application of ultra-high voltage components.
雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention. Anyone with ordinary knowledge in the relevant technical field can make some changes and modifications without departing from the spirit and scope of the present invention. The scope of protection of the present invention shall be determined by the scope of the attached patent application.
10:半導體裝置10: Semiconductor device
100:基板100: substrate
102:高壓井102: high pressure well
104:源極井104: Source Well
104a、108a:邊緣部分104a, 108a: edge part
106:汲極井106: Kick Well
108:隔離層108: isolation layer
110:閘極層110: gate layer
112:源極區112: source region
114:汲極區114: Drain Region
116、300a、300b:浮置導體層116, 300a, 300b: floating conductor layer
118:第一重摻雜區118: The first heavily doped region
120:第二重摻雜區120: second heavily doped region
122:場氧化層122: Field Oxide
124:飄移區124: Drift Zone
126:頂區126: Top Zone
128:梯度區128: gradient zone
400:突升區400: Sudden rise area
s1、s2:距離s1, s2: distance
t1、t2:厚度t1, t2: thickness
w1、w2、w3:寬度w1, w2, w3: width
圖1是依照本發明的一實施例的一種半導體裝置的俯視示意圖。 圖2是圖1的II-II’線段的半導體裝置的剖面示意圖。 圖3是依照本發明的另一實施例的一種半導體裝置的剖面示意圖。 圖4是圖2的半導體裝置的隔離層下方的電場分布圖。 圖5是實驗例1與比較例1隨N型高壓井的劑量比例變化的崩潰電壓曲線圖。 圖6是實驗例2與比較例2隨P型頂區的劑量比例變化的崩潰電壓曲線圖。 圖7是實驗例1、實驗例2與沒有浮置導體層且N型高壓井和P型頂區的劑量均為標準值的Ron曲線圖。 FIG. 1 is a schematic top view of a semiconductor device according to an embodiment of the invention. FIG. 2 is a schematic cross-sectional view of the semiconductor device along the line II-II' of FIG. 1. FIG. 3 is a schematic cross-sectional view of a semiconductor device according to another embodiment of the invention. 4 is a diagram of the electric field distribution under the isolation layer of the semiconductor device of FIG. 2. Figure 5 is a graph showing the breakdown voltage curves of Experimental Example 1 and Comparative Example 1 with the dose ratio of the N-type high-pressure well. Fig. 6 is a graph showing the breakdown voltage curve of Experimental Example 2 and Comparative Example 2 with the variation of the dose ratio of the P-type top zone. Fig. 7 is a Ron curve diagram of experimental example 1, experimental example 2, and no floating conductor layer and the doses of the N-type high pressure well and the P-type top zone are all standard values.
10:半導體裝置 10: Semiconductor device
100:基板 100: substrate
102:高壓井 102: high pressure well
104:源極井 104: Source Well
104a、108a:邊緣部分 104a, 108a: edge part
106:汲極井 106: Kick Well
108:隔離層 108: isolation layer
110:閘極層 110: gate layer
112:源極區 112: source region
114:汲極區 114: Drain Region
116:浮置導體層 116: floating conductor layer
118:第一重摻雜區 118: The first heavily doped region
120:第二重摻雜區 120: second heavily doped region
122:場氧化層 122: Field Oxide
124:飄移區 124: Drift Zone
126:頂區 126: Top Zone
128:梯度區 128: gradient zone
s1、s2:距離 s1, s2: distance
t1、t2:厚度 t1, t2: thickness
w1:寬度 w1: width
Claims (7)
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| TW201310642A (en) * | 2011-08-25 | 2013-03-01 | United Microelectronics Corp | High voltage metal-oxide-semiconductor transistor device and method of fabricating the same |
| TW201601315A (en) * | 2014-06-18 | 2016-01-01 | 旺宏電子股份有限公司 | Semiconductor device having metal layer over drift region |
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| TW201310642A (en) * | 2011-08-25 | 2013-03-01 | United Microelectronics Corp | High voltage metal-oxide-semiconductor transistor device and method of fabricating the same |
| TW201601315A (en) * | 2014-06-18 | 2016-01-01 | 旺宏電子股份有限公司 | Semiconductor device having metal layer over drift region |
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