TWI692866B - Semiconductor element, semiconductor substrate and semiconductor element manufacturing method - Google Patents
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- 238000009792 diffusion process Methods 0.000 claims abstract description 44
- 238000000034 method Methods 0.000 claims description 24
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- 229910052698 phosphorus Inorganic materials 0.000 description 13
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- 238000005516 engineering process Methods 0.000 description 8
- 230000000694 effects Effects 0.000 description 7
- 239000011521 glass Substances 0.000 description 7
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 7
- 238000011084 recovery Methods 0.000 description 7
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 4
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 4
- 229910052796 boron Inorganic materials 0.000 description 4
- 238000009826 distribution Methods 0.000 description 4
- 238000005265 energy consumption Methods 0.000 description 4
- 239000010931 gold Substances 0.000 description 4
- 238000002161 passivation Methods 0.000 description 4
- 239000011574 phosphorus Substances 0.000 description 4
- 230000015572 biosynthetic process Effects 0.000 description 3
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 3
- 229910052737 gold Inorganic materials 0.000 description 3
- 229910052697 platinum Inorganic materials 0.000 description 3
- 230000006798 recombination Effects 0.000 description 3
- 238000005215 recombination Methods 0.000 description 3
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 238000013467 fragmentation Methods 0.000 description 2
- 238000006062 fragmentation reaction Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
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- 210000004508 polar body Anatomy 0.000 description 1
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- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/0684—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape, relative sizes or dispositions of the semiconductor regions or junctions between the regions
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- H01L29/66083—Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by variation of the electric current supplied or the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched, e.g. two-terminal devices
- H01L29/6609—Diodes
- H01L29/66136—PN junction diodes
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/86—Types of semiconductor device ; Multistep manufacturing processes therefor controllable only by variation of the electric current supplied, or only the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched
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Abstract
一種半導體元件,包含:一基板,該基板具有一第一表面及一第二表面;一凹部,形成於該第一表面上;及一第一摻雜區,其係藉由在具有該凹部之該第一表面進行熱擴散處理而形成於該基板內,其中,該第一摻雜區對應於該凹部之部分與該第二表面之最短距離小於該第一摻雜區對應於該第一表面之非凹部之部分與該第二表面之最短距離。 A semiconductor device includes: a substrate having a first surface and a second surface; a concave portion formed on the first surface; and a first doped region formed by the concave portion The first surface is formed in the substrate by thermal diffusion, wherein the shortest distance between the portion of the first doped region corresponding to the recess and the second surface is smaller than that of the first doped region corresponding to the first surface The shortest distance between the non-recessed portion and the second surface.
Description
本發明係有關於半導體元件、用以製作該半導體元件之基板、及該半導體元件之製作方法,特別是關於一種具有凹部之半導體元件、用以製作該具有凹部之半導體元件之基板、及該具有凹部之半導體元件之製作方法。 The invention relates to a semiconductor element, a substrate for manufacturing the semiconductor element, and a method for manufacturing the semiconductor element, in particular to a semiconductor element with a recess, a substrate for manufacturing the semiconductor element with a recess, and the A method for manufacturing a semiconductor element in a recess.
習知的一種PN二極體結構,是在基板的兩面分別藉由熱擴散處理將P摻雜(例如硼或其他III A族元素)與N摻雜(例如磷或其他IV A族元素)驅入(drive-in)基板,此處理過程需要長時間以及高溫,因此耗費的能量極高,是二極體元件整個製作過程中最為耗能的階段。一般而言,在摻雜驅入的熱擴散處理中,溫度通常高於攝氏1100度,時間常超過150小時,而P摻雜或N摻雜的驅入深度只能達到約150~180微米(μm)。 A conventional PN diode structure is to drive P doping (such as boron or other group III A elements) and N doping (such as phosphorus or other group IV A elements) by thermal diffusion treatment on both sides of the substrate. In the drive-in substrate, this process requires a long time and high temperature, so the energy consumption is extremely high, which is the most energy-consuming stage in the entire manufacturing process of the diode element. In general, in the thermal diffusion process of doping drive, the temperature is usually higher than 1100 degrees Celsius, the time is often more than 150 hours, and the driving depth of P doping or N doping can only reach about 150 ~ 180 microns ( μm).
為了讓晶圓維持一定的機械強度,以避免在元件製作過程中破裂或破碎,業界的實際製程中通常4吋晶圓至少需要有350~400微米的厚度,以避免製程中發生破片的情形而造成良率降低。 In order to maintain a certain mechanical strength of the wafer to avoid cracking or breaking during device manufacturing, the industry's actual process usually requires a 4-inch wafer to have a thickness of at least 350 to 400 microns to avoid fragmentation during the process Cause yield reduction.
一般而言,磷摻雜與硼摻雜藉由熱擴散的最大深度約為150微米,若晶圓厚度大於300微米,在晶圓兩面分別進行磷摻雜與硼摻雜的熱擴散之後,都會留下未受到二次高溫驅入摻雜的區 域。晶圓厚度分別減去磷摻雜與硼摻雜的擴散深度後,即為未二次摻雜區域的厚度或寬度,此數值又稱為基寬(base width)。 In general, the maximum depth of thermal diffusion of phosphorus doping and boron doping is about 150 microns. If the thickness of the wafer is greater than 300 microns, the thermal diffusion of phosphorus doping and boron doping on both sides of the wafer will be Leaving a region that is not doped by secondary high temperature drive area. The thickness of the wafer minus the diffusion depth of phosphorus doping and boron doping is the thickness or width of the non-secondary doped region. This value is also called the base width.
根據波松方程式(Poisson’s equation),PN接面電荷濃度及基寬會影響二極體元件的電壓表現。另一方面,未二次摻雜區域為二極體元件中阻抗最高的區域,除了支持電壓,同時也會造成電流導通的阻抗。換言之,基寬越大,二極體元件工作時的導通能量損耗也會越高。因此在設計元件結構時,必須嚴格地控制基寬,以控制二極體元件的順向電壓(forward voltage;VF)與反向電壓(reverse voltage;VR)之特性。習知技術中一般是使用磊晶晶圓(Epi wafer),在一較高摻雜之厚基板上形成較低摻雜的磊晶半導體層(epi layer),以提供足夠的基板厚度(機械強度),並設定基寬(前述磊晶半導體層的厚度為摻雜深度加上支持所設定之反向偏壓的基寬)來支持元件的電壓表現及最低阻抗。 According to Poisson's equation, the charge concentration and base width of the PN junction will affect the voltage performance of the diode element. On the other hand, the non-secondary doped region is the region with the highest impedance among the diode elements. In addition to supporting the voltage, it will also cause the impedance of current conduction. In other words, the larger the base width, the higher the conduction energy loss when the diode element works. Therefore, when designing the device structure, the base width must be strictly controlled to control the characteristics of the forward voltage (V F ) and reverse voltage (V R ) of the diode device. In the conventional technology, an epi wafer is generally used to form a lower doped epi layer on a thicker doped substrate to provide sufficient substrate thickness (mechanical strength) ), and set the base width (the thickness of the epitaxial semiconductor layer is the doping depth plus the base width that supports the set reverse bias) to support the voltage performance and the lowest impedance of the device.
此外,對於具有快速恢復(recovery)特性的二極體元件設計而言,習知的一種方式是將載子生命週期殺手(lifetime killer)摻雜至元件中,使其分布於PN接面附近之區域,當二極體元件從順向偏壓模式切換到反向偏壓模式時,元件中摻雜的載子生命週期殺手可加速PN接面附近剩餘電荷(即電子及電洞)的復合,從而縮短電流完全切斷所需的時間,亦即反向恢復時間(reverse recovery time)。 In addition, for the design of diode devices with fast recovery characteristics, a common way is to dope the life cycle killer of the carrier into the device so that it is distributed near the PN junction In the region, when the diode element switches from forward bias mode to reverse bias mode, the life cycle killer of the carrier doped in the element can accelerate the recombination of the remaining charges (ie, electrons and holes) near the PN junction. This shortens the time required for the current to be completely cut off, that is, the reverse recovery time.
載子生命週期殺手的摻雜,一般是從晶圓表面(P摻雜或N摻雜之表面)將鉑(Pt)或金(Au)以熱擴散方式進行摻雜。由於剩餘電荷主要存在於PN接面附近,為了有效地加速二極體內剩餘電荷的復合,須使鉑或金摻雜也分布在PN接面附近。因此,具 有越深PN接面之二極體元件便需要更高溫的熱擴散處理,才足以將更高濃度的載子生命週期殺手趨入至更深的PN接面附近,使其加速電子與電洞的復合。相對地,若無法將足夠的載子生命週期殺手驅入足夠的深度,將無法有效地縮短二極體元件的反向恢復時間。 Carrier life cycle killer doping is generally doping platinum (Pt) or gold (Au) from the wafer surface (P-doped or N-doped surface) by thermal diffusion. Since the residual charge mainly exists near the PN junction, in order to effectively accelerate the recombination of the residual charge in the diode, platinum or gold doping must also be distributed near the PN junction. Therefore, with Diode components with deeper PN junctions require higher temperature thermal diffusion treatment, which is enough to move the higher concentration carrier life cycle killer to the deeper PN junction, so that it accelerates the electrons and holes. complex. On the contrary, if the carrier life cycle killer cannot be driven to a sufficient depth, the reverse recovery time of the diode element cannot be effectively shortened.
綜上所述,對二極體元件的製造而言,為了維持機械強度及製程良率,晶圓基板必須有一定的厚度,此時若欲縮小基寬以降低元件的阻抗,就必須提高熱擴散處理的溫度及/或時間,使摻雜能被驅入到足夠的深度,如此不但使得製程非常耗能,也不利於進一步以摻雜載子生命週期殺手的手段來縮短二極體元件的反向回復時間。因此,過去在設計二極體元件時並無法突破上述這些限制,只能視情況折衷,也缺乏控制元件參數的彈性。 In summary, for the manufacture of diode devices, in order to maintain the mechanical strength and process yield, the wafer substrate must have a certain thickness. If you want to reduce the base width to reduce the resistance of the device, you must increase the heat. The temperature and/or time of the diffusion process enables the doping to be driven to a sufficient depth, which not only makes the process very energy-intensive, but also not conducive to further shortening the diode element with the killer of the doping carrier life cycle Reverse reply time. Therefore, in the past, when designing diode components, these limitations could not be overcome. They could only be compromised according to the situation, and they lacked the flexibility to control the parameters of the components.
針對先前技術所存在的問題,本發明提出一種具有凹部結構的二極體元件,其製作方式是在晶圓基板上先形成凹部後,再進行熱擴散處理。因此,在對應於凹部的區域,P摻雜區域與N摻雜區域的距離會縮短,從而等效地減少整個元件的基寬。或者說,只需要較淺的P、N摻雜區便可得到與習知不具凹部之二極體元件相當之電壓/電流表現,可大幅降低熱擴散處理時所需耗費的能源。 In view of the problems existing in the prior art, the present invention proposes a diode element with a recessed structure. The manufacturing method is to form a recessed portion on a wafer substrate before performing a thermal diffusion process. Therefore, in the region corresponding to the recess, the distance between the P-doped region and the N-doped region is shortened, thereby equivalently reducing the base width of the entire device. In other words, only shallower P and N doped regions are needed to obtain voltage/current performance equivalent to conventional diode devices without recesses, which can greatly reduce the energy consumption required for thermal diffusion treatment.
本發明的一個面向是提供一種半導體元件,其包含一基板,此基板具有一第一表面及一第二表面,該第一表面上具有一凹部;此半導體元件並包含一第一摻雜區,此第一摻雜區是藉由在具有該凹部之該第一表面進行熱擴散處理而形成於該基板內,使該 第一摻雜區對應於該凹部之部分與該第二表面之最短距離小於該第一摻雜區對應於該第一表面之非凹部之部分與該第二表面之最短距離。在此半導體元件中,可進一步包含一第二摻雜區,其係藉由在該第二表面進行熱擴散處理而形成於該基板內。此外,該凹部可以例如是圓柱形之空間。 An aspect of the present invention is to provide a semiconductor device including a substrate having a first surface and a second surface with a concave portion on the first surface; the semiconductor device also includes a first doped region, The first doped region is formed in the substrate by thermal diffusion treatment on the first surface having the recess, so that the The shortest distance between the portion of the first doped region corresponding to the recess and the second surface is less than the shortest distance between the portion of the first doped region corresponding to the non-recessed portion of the first surface and the second surface. In this semiconductor device, a second doped region may be further included, which is formed in the substrate by thermal diffusion treatment on the second surface. Furthermore, the recess can be, for example, a cylindrical space.
本發明的另一個面向是提供一種用於製作複數半導體元件之半導體基板,其包含一晶圓,該晶圓具有一第一表面及一第二表面;並包含複數凹部,係藉由蝕刻處理而形成於該第一表面,該等凹部的位置對應於所欲製作之該等二極體元件的位置(或特定相對位置)。在此半導體基板中,該等凹部可以例如是圓柱形空間。 Another aspect of the present invention is to provide a semiconductor substrate for manufacturing a plurality of semiconductor devices, which includes a wafer having a first surface and a second surface; and includes a plurality of concave portions, which are processed by etching Formed on the first surface, the positions of the recesses correspond to the positions (or specific relative positions) of the diode elements to be manufactured. In this semiconductor substrate, the recesses may be, for example, cylindrical spaces.
使用如前段所述之半導體基板,本發明的另一個面向是提供一種半導體元件之製作方法,其步驟中包含對該半導體基板之第一表面進行熱擴散處理,使該半導體基板內形成一第一摻雜區,此第一摻雜區對應於該等凹部之部分與該第二表面之最短距離小於該第一摻雜區對應於該第一表面之非凹部之部分與該第二表面之最短距離。此處所述之半導體元件之製作方法中,可在形成該第一摻雜區之前或之後,藉由對該半導體基板之該第二表面進行熱擴散處理,使該半導體基板內形成一第二摻雜區,並可進一步在形成該第一摻雜區及該第二摻雜區之後,藉由對該半導體基板之該第一或第二表面進行熱擴散處理,使載子生命週期殺手被驅入該半導體基板內。 Using the semiconductor substrate as described in the previous paragraph, another aspect of the present invention is to provide a method for manufacturing a semiconductor element, the steps of which include performing thermal diffusion treatment on the first surface of the semiconductor substrate to form a first in the semiconductor substrate A doped region, the shortest distance between the portion of the first doped region corresponding to the recesses and the second surface is less than the shortest distance between the portion of the first doped region corresponding to the non-recessed portion of the first surface and the second surface distance. In the manufacturing method of the semiconductor device described herein, before or after the formation of the first doped region, by performing thermal diffusion treatment on the second surface of the semiconductor substrate, a second A doped region, and further after forming the first doped region and the second doped region, by performing thermal diffusion treatment on the first or second surface of the semiconductor substrate, the carrier life cycle killer is Drive into the semiconductor substrate.
因此,根據本發明,至少可達成以下無法預期之功效:(1)藉由適當設計凹部的幾何結構,例如形狀、深度、寬度... 等,可以更有效且更有彈性地控制二極體元件的電壓/電流特性,亦可更有彈性地調整製程中的其他步驟或條件;(2)在傳統二極體元件中加入凹部結構,可以降低二極體元件的順向電壓VF,亦即可降低元件的能量傳輸損耗;(3)具有凹部結構之二極體元件,在P、N摻雜深度相對較淺的情況下,就可達到與不具凹部結構之二極體元件相當的電壓/電流特性,因此可降低熱擴散處理時設備的耗能,並減少熱擴散處理所需要的時間,從而提升生產效率;(4)凹部結構若應用在快速恢復二極體上,由於PN接面的深度相對較淺,載子生命週期殺手所需要的驅入深度也降低,使得載子生命週期殺手的熱擴散處理之時間縮短、溫度降低,並且可縮短二極體元件的反向恢復時間;(5)加入凹部結構仍維持足夠的晶圓機械強度,避免製程中發生破片的情況。換言之,在實現上述功效的同時,不需要犧牲機械強度及製程良率。此外,具有凹部結構的PN二極體元件在進行玻璃鈍化處理(glass passivation process;GPP)時,所需形成之溝槽深度相對較淺,亦可相對地提升晶圓機械強度與製程良率。 Therefore, according to the present invention, at least the following unexpected effects can be achieved: (1) By appropriately designing the geometry of the recess, such as shape, depth, width, etc., the diode can be controlled more effectively and more elastically The voltage/current characteristics of the device can also be used to adjust other steps or conditions in the manufacturing process more flexibly; (2) Adding a recess structure to the traditional diode device can reduce the forward voltage V F of the diode device. It can reduce the energy transmission loss of the element; (3) The diode element with a concave structure can reach a voltage equivalent to the diode element without a concave structure when the P and N doping depths are relatively shallow / Current characteristics, so it can reduce the energy consumption of the device during thermal diffusion treatment and reduce the time required for thermal diffusion treatment, thereby improving production efficiency; (4) If the concave structure is applied to the rapid recovery diode, due to the PN junction The depth of the carrier is relatively shallow, and the driving depth required by the carrier life cycle killer is also reduced, which shortens the time and temperature of the thermal diffusion treatment of the carrier life cycle killer, and can shorten the reverse recovery time of the diode element; (5) Adding the concave structure still maintains sufficient mechanical strength of the wafer to avoid fragmentation during the manufacturing process. In other words, while achieving the above-mentioned effects, there is no need to sacrifice mechanical strength and process yield. In addition, when a PN diode device with a concave structure is subjected to a glass passivation process (GPP), the depth of the trench to be formed is relatively shallow, which can also relatively improve the mechanical strength of the wafer and the yield of the process.
1‧‧‧半導體基板 1‧‧‧Semiconductor substrate
2‧‧‧晶圓 2‧‧‧ Wafer
10‧‧‧凹部 10‧‧‧recess
11‧‧‧第一摻雜區域 11‧‧‧First doped region
12‧‧‧第二摻雜區域 12‧‧‧Second doped region
13‧‧‧第一摻雜區域 13‧‧‧First doped region
14‧‧‧第二摻雜區域 14‧‧‧Second doped region
15‧‧‧載子生命週期殺手驅入深度 15‧‧‧ Carrier life cycle killer drives deeper
16‧‧‧溝槽 16‧‧‧groove
20‧‧‧凹部 20‧‧‧recess
101‧‧‧第一凹部 101‧‧‧First recess
102‧‧‧第二凹部 102‧‧‧Second recess
D1‧‧‧距離 D1‧‧‧Distance
D2‧‧‧距離 D2‧‧‧Distance
圖1為習知二極體元件之局部結構示意圖;圖2(a)為本發明之具有凹部之半導體基板之示意圖;圖2(b)為本發明之具有凹部之二極體元件之局部結構之示意圖;圖2(c)為本發明之具有兩個凹部之二極體元件之局部結構之示 意圖;圖3為本發明之具有複數凹部之晶圓之示意圖;圖4(a)為用於進行電腦模擬之先前技術之二極體元件結構之示意圖;圖4(b)為用於進行電腦模擬之本發明之二極體元件結構之示意圖;圖4(c)為用於進行電腦模擬之另一先前技術之二極體元件結構之示意圖;圖5為圖4(a)、(b)、(c)所示之結構之順向電壓之電腦模擬結果;圖6為圖4(a)、(b)、(c)所示之結構之反向電壓之電腦模擬結果;圖7為本發明之二極體結構進行載子生命週期殺手驅入之示意圖;圖8為本發明之二極體結構進行玻璃鈍化處理之示意圖。 FIG. 1 is a schematic diagram of a partial structure of a conventional diode device; FIG. 2(a) is a schematic diagram of a semiconductor substrate with recesses of the present invention; FIG. 2(b) is a partial structure of a diode device of the present invention with recesses 2(c) is a partial structure diagram of a diode element with two recesses according to the present invention FIG. 3 is a schematic diagram of a wafer with a plurality of recesses of the present invention; FIG. 4(a) is a schematic diagram of a prior art diode device structure used for computer simulation; FIG. 4(b) is used for computer A schematic diagram of the structure of the diode element of the present invention simulated; FIG. 4(c) is a schematic diagram of another prior art diode element structure used for computer simulation; FIG. 5 is FIG. 4(a), (b) , (C) The computer simulation results of the forward voltage of the structure shown in Figure 6; Figure 6 is the computer simulation results of the reverse voltage of the structure shown in Figure 4 (a), (b), (c); Figure 7 is based on The schematic diagram of the invention's diode structure is driven by the killer of the carrier life cycle; Figure 8 is a schematic diagram of the invention's diode structure subjected to glass passivation treatment.
本發明之具體實施方式將配合圖式說明如下。其中,圖式所呈現之結構或幾何關係僅為示意之目的,不代表實際裝置或元件之結構或幾何,也不用於限制裝置或元件的所有組成。例如,使用熱擴散處理在半導體基板中形成之P、N摻雜區域,其摻雜濃度並非均勻分布,實際上與基板中之未摻雜區域並無明顯之界線。惟若設定一摻雜濃度的臨界值,則可界定出摻雜區域之邊界。同理,由於摻雜區域的幾何或結構並不易以文字加以描述,在描述摻雜區域時(例如在申請專利範圍中),以製造方法(例如熱擴散處理)加以界定乃是更適當的方式,因為摻雜的分布會取決於摻雜與基板材料的性質、擴散溫度與時間...等條件,此為習知之通常知 識,本發明所屬技術領域中具有通常知識者亦可由材料與製程條件輕易地推知其所對應形成之元件結構或幾何。 The specific embodiments of the present invention will be described in conjunction with the drawings as follows. The structure or geometric relationship presented in the drawings is for illustrative purposes only, and does not represent the structure or geometry of the actual device or element, nor is it used to limit all components of the device or element. For example, the doping concentration of the P and N doped regions formed in the semiconductor substrate by thermal diffusion treatment is not uniformly distributed, and in fact there is no obvious boundary with the undoped regions in the substrate. However, if a critical value of the doping concentration is set, the boundary of the doping area can be defined. Similarly, because the geometry or structure of the doped region is not easy to describe in words, when describing the doped region (such as in the patent application), it is more appropriate to define it by the manufacturing method (such as thermal diffusion treatment) , Because the distribution of doping will depend on the properties of the doping and substrate materials, diffusion temperature and time, etc., which is commonly known It can be understood that those with ordinary knowledge in the technical field of the present invention can also easily deduce the corresponding device structure or geometry formed from the materials and process conditions.
圖1為傳統二極體元件之局部示意圖,其中半導體基板1可例如是矽(Si)晶圓,可使用經摻雜或不經摻雜之矽晶圓。傳統二極體元件的一種製作方式,是藉由熱擴散處理在半導體基板1的兩個表面分別進行P、N摻雜,而形成圖1所示之第一摻雜區域11及第二摻雜區域12。如前所述,若要維持良率並使P、N摻雜區域的距離(基寬)足夠小,就必須讓P、N摻雜被驅入至足夠的深度,亦即需要較大的擴散深度來形成深接面的二極體元件。對此,圖2為本發明提出的二極體元件及其製作方法之示意圖。有別於圖1之傳統二極體結構,本發明係在半導體基板1上形成一凹部10,如圖2(a)所示。然後,在半導體基板1的兩個表面進行P、N摻雜的熱擴散處理,以形成第一摻雜區域13及第二摻雜區域14,如圖2(b)所示。
FIG. 1 is a partial schematic diagram of a conventional diode device, wherein the
如圖3所示,在實際製程中,具有凹部10之基板是對晶圓2進行蝕刻而形成複數個凹部20,然後進行後續的其他製程。因此,這些凹部20可對應於每個晶粒(die)的位置。
As shown in FIG. 3, in the actual manufacturing process, the substrate with the recessed
由圖2(b)可看出,本發明之二極體之結構特徵主要在於第一摻雜區域13的分布。由於先形成凹部10後再進行熱擴散處理,第一摻雜區域13與第二摻雜區域14在對應凹部之部分會具有較近的距離D2,D2小於第一摻雜區域13與第二摻雜區域14在對應非凹部之部分的距離D1。換言之,藉由凹部10的幾何結構,可以控制第一摻雜區域13與第二摻雜區域14之間一部份的距離。須注意的是,圖2中所呈現之凹部10之截面為矩形,其對應之立體
結構可能是圓柱形空間或長方體空間,又矩形截面僅為本發明之凹部10的其中一種實施方式,其截面形狀並不限為矩形,例如可為倒三角形或倒半圓形。除了形狀,其幾何尺寸(例如深度、寬度)也可以依需求進行適當的選擇,本發明所屬技術領域中具有通常知識者可自行加以適當地設計。此外,圖2雖然僅揭示在半導體基板1的一個表面形成一個凹部10,惟亦有可能在一個二極體元件(晶粒)的一個表面形成兩個以上的凹部、或是在兩個表面均形成凹部,再進行摻雜的熱擴散處理。例如,在二極體元件之橫向(圖2(b)之水平方向)尺寸較大的情況,若形成單一個凹部無法同時滿足所欲之電壓特性及機械強度時,可在單一個晶粒上形成兩個以上的凹部,每個凹部可具有相同或不同的幾何結構,藉此增加更多的設計彈性,實現單一個凹部所無法兼顧的電壓特性及機械強度。圖2(c)呈現在單一二極體元件中具有兩個凹部之結構示意圖,根據載子導通或復合的需求,其中兩個凹部可設計為空間上對稱或不對稱,並且兩個凹部可具有相同或不同之形狀與幾何結構(如圖2(c)所示之截面,第一凹部101與第二凹部102為矩形截面,惟寬度可不同,且兩個凹部相對於圖2(c)之橫向中心點可非對稱地設置;若從圖2(c)上方俯視,第一凹部101與第二凹部102可為非相同大小之特定分布)。
As can be seen from FIG. 2(b), the structural feature of the diode of the present invention is mainly the distribution of the first
本發明之實施方式中,凹部的形成及摻雜的熱擴散處理均為習知的半導體製造技術,即使本說明書中並未就製程細節與參數詳加說明,本發明所屬技術領域中具有通常知識者當可基於習知技術而加以實現。例如,對PN二極體而言,凹部可依照元件與製程特性選擇形成於P摻雜之表面或N摻雜之表面。 In the embodiments of the present invention, the formation of recesses and the thermal diffusion treatment of doping are conventional semiconductor manufacturing technologies. Even though the process details and parameters are not described in detail in this specification, the technical field of the present invention has general knowledge They should be implemented based on conventional technology. For example, for a PN diode, the recess can be formed on the P-doped surface or the N-doped surface according to the device and process characteristics.
本發明提出之具有凹部的二極體元件,藉由在基板上形成凹部而改變至少一摻雜區域的分佈,從而可改變二極體元件的特性。以下將以電壓/電流的表現為例,藉由電腦模擬的方式呈現本發明對於提升二極體元件特性之功效。圖4(a)至圖4(c)為進行電腦模擬所使用之元件結構:圖4(a)為習知技術的二極體元件結構;圖4(b)為本發明之具有凹部的二極體元件結構,其摻雜之熱擴散處理的溫度及時間與圖4(a)相同;圖4(c)亦為習知技術之二極體元件結構,惟其相較於圖4(a)使用更高溫及更長時間的摻雜之熱擴散處理,因此相較於圖4(a)其摻雜擴散深度更深、基寬更小。在圖4(a)至圖4(c)中,橫軸與縱軸的單位均為微米,各元件之摻雜極性如圖中所示。根據圖4(a)至圖4(c)的三種結構,圖5為電腦模擬所得到之順向偏壓特性。由圖5可看出,本發明之元件結構(圖4(b))相較於使用相同摻雜擴散條件之習知二極體元件(圖4(a)),可以大幅地降低順向電壓VF(順向偏壓時的導通壓降)。而即使大幅度地加深習知二極體元件中之摻雜擴散深度(圖4(c)),其VF仍高於本發明。換言之,本發明之具有凹部之二極體元件,可以在相同的摻雜擴散條件(相當於同等耗能程度)下,得到更低的VF;且習知技術即使摻雜的擴散深度更深(相當於更耗能),其降低VF的效果仍不及本發明。另一方面,圖6顯示本發明之元件結構在反向偏壓時所呈現的電壓/電流特性與習知技術並無明顯之差異。基於相同原理,對本發明所屬技術領域具有通常知識者而言,可以預期包含兩個以上凹部的二極體元件(例如圖2(c)所示者)也會具有類似的電壓/電流特性,且多個凹部更可增加設計上的彈性,例如但不限於:順向電流密度的控制(電流密度與導通阻抗密切相關),或者藉由 較小的凹部設計(或局部無凹部)提升晶粒特定部位之機械強度。 The diode element provided with recesses in the present invention can change the distribution of at least one doped region by forming recesses on the substrate, so that the characteristics of the diode element can be changed. The following will take the performance of voltage/current as an example to present the effect of the present invention on improving the characteristics of diode elements by way of computer simulation. 4(a) to 4(c) are element structures used for computer simulation: FIG. 4(a) is a diode element structure of the conventional technology; FIG. 4(b) is a diode with a recess in the present invention. For the structure of the polar body, the temperature and time of the thermal diffusion treatment of the doping are the same as those in FIG. 4(a); FIG. 4(c) is also the structure of the diode body of the conventional technology, but it is compared with FIG. 4(a) A higher temperature and longer time doping thermal diffusion process is used, so the doping diffusion depth is deeper and the base width is smaller compared to FIG. 4(a). In FIGS. 4(a) to 4(c), the units of the horizontal axis and the vertical axis are both micrometers, and the doping polarity of each element is shown in the figure. According to the three structures of FIG. 4(a) to FIG. 4(c), FIG. 5 is the forward bias characteristics obtained by computer simulation. It can be seen from FIG. 5 that the device structure of the present invention (FIG. 4(b)) can greatly reduce the forward voltage compared to the conventional diode device using the same doping and diffusion conditions (FIG. 4(a)). V F (on-voltage drop in forward bias). Even if the doping diffusion depth in the conventional diode device is greatly increased (FIG. 4(c)), the V F is still higher than that of the present invention. In other words, the diode element of the present invention having a concave portion can obtain a lower V F under the same doping and diffusion conditions (equivalent to the same energy dissipation degree); and the conventional technology even if the doping diffusion depth is deeper ( Equivalent to more energy consumption), its effect of reducing V F is still not as good as the present invention. On the other hand, FIG. 6 shows that the voltage/current characteristics of the device structure of the present invention when reverse-biased are not significantly different from the conventional technology. Based on the same principle, for those with ordinary knowledge in the technical field to which the present invention belongs, it can be expected that a diode element including more than two recesses (such as the one shown in FIG. 2(c)) will also have similar voltage/current characteristics, and Multiple recesses can increase the design flexibility, such as but not limited to: control of forward current density (current density is closely related to on-resistance), or improve die specificity through smaller recess design (or partial absence of recesses) The mechanical strength of the part.
由前段說明可知,本發明之具有凹部的二極體元件確實可以改善(或者至少改變)元件的特性。因此,在實際的元件設計過程中,藉助於電腦模擬技術,本發明之凹部結構可針對應用領域、預期之元件特性、製程能力、成本...等考量加以變化,而得到有效達成目的之元件結構與製程條件參數。換言之,對本發明所屬技術領域中具有通常知識者而言,透過簡單嘗試即可決定出最佳或者最合適的元件結構與製程條件參數。在實際製程中,由於蝕刻、熱擴散處理、元件結構與特性的測量等技術均已十分成熟,本發明所屬技術領域中具有通常知識者也僅需要簡單嘗試,即可實現本發明之結構並驗證其效果。 As can be seen from the foregoing description, the diode element of the present invention having a recess can indeed improve (or at least change) the characteristics of the element. Therefore, in the actual device design process, with the help of computer simulation technology, the concave structure of the present invention can be changed according to the application field, expected device characteristics, process capability, cost, etc., to obtain a device that effectively achieves the purpose Structure and process condition parameters. In other words, for those with ordinary knowledge in the technical field to which the present invention belongs, a simple trial can determine the best or most suitable device structure and process condition parameters. In the actual manufacturing process, since the techniques of etching, thermal diffusion treatment, measurement of device structure and characteristics are all very mature, those with ordinary knowledge in the technical field of the present invention only need to simply try to realize the structure of the present invention and verify Its effect.
除了電壓/電流特性之外,以下進一步說明本發明之具有凹部的二極體元件所具有之其他功效。 In addition to the voltage/current characteristics, the following further describes other functions of the diode element with recesses of the present invention.
為了使二極體元件具有快速回復的特性,習知的一種作法是將載子生命週期殺手(例如金或鉑)摻雜至元件的PN接面附近。若將圖2(b)所示之具有凹部的二極體元件結構藉由熱擴散處理進行載子生命週期殺手之摻雜,可形成如圖7所示之結構;其中,上圖、下圖分別顯示從兩個表面進行擴散之驅入深度15。本發明之二極體元件對於載子生命週期殺手之摻雜的有益效果至少有兩方面。首先,表面的凹部結構可以讓載子生命週期殺手更容易被驅入至理想的深度;其次,具有凹部結構之二極體元件,可以採用較淺的PN摻雜區域,因此載子生命週期殺手也對應地只需要被驅入至較淺的深度。再者,凹部結構可以形成於晶粒範圍的特定區域及深度,亦有助於將載子生命週期殺手摻雜到特定的位置,產生所欲之
特定的晶粒反向回復時間及波形。因此,配合前述之說明,本發明藉由在二極體元件上形成凹部,除了可以視需要控制凹部形成之條件(例如但不限於:形成於P或N摻雜之表面、凹部數量、每一凹部之幾何結構等),並可進一步控制載子生命週期殺手的摻雜條件(例如但不限於:從有凹部或無凹部之表面進行擴散、從P或N摻雜之表面進行擴散、擴散溫度及時間等),來實現所欲之元件特性。
In order to make the diode device have the characteristics of fast recovery, a common practice is to dope the carrier life cycle killer (such as gold or platinum) near the PN junction of the device. If the diode element structure with recesses shown in FIG. 2(b) is doped by the life-cycle killer of the carrier through thermal diffusion treatment, the structure shown in FIG. 7 can be formed; Respectively show the
在習知的二極體製造過程中,可以加入玻璃鈍化製程(glass passivation process;GPP),主要包含形成溝槽並填入玻璃,而形成如圖8所示之元件結構。其中,用於填入玻璃之溝槽16的深度會受到第二摻雜區域14之深度的影響。如前所述,本發明提出之具有凹部的二極體元件,可降低第二摻雜區域14之深度,從而降低溝槽16所需的深度。在玻璃鈍化過程中形成較淺的溝槽,除了可相對提高製程的良率,在使用濕式蝕刻形成溝槽時,較深的溝槽容易在溝槽頂部形成鳥嘴狀而導致玻璃附著或包覆效果不良,而較淺的溝槽則可避免這些問題。
In the conventional diode manufacturing process, a glass passivation process (GPP) can be added, which mainly includes forming a trench and filling the glass to form the device structure shown in FIG. 8. Among them, the depth of the
以上所述僅為本發明實施方式與功效之例示,並非窮盡列舉所有可能之變化。根據本發明之概念,本發明所屬技術領域中具有通常知識者,自可依據本說明書揭露之內容自行變化而輕易實現本發明之概念所涵蓋的各種具體變化。申請人主張之權利範圍如後述申請專利範圍所載,其中各請求項之文義及均等範圍均為本專利之權利範圍所涵蓋。 The above is only an example of the embodiments and effects of the present invention, and it is not exhaustive to list all possible changes. According to the concept of the present invention, those with ordinary knowledge in the technical field to which the present invention pertains can easily make various specific changes covered by the concept of the present invention by changing themselves according to the contents disclosed in this specification. The scope of rights claimed by the applicant is set out in the scope of patent application mentioned later, in which the meaning and the equal scope of each claim are covered by the scope of rights of this patent.
1‧‧‧半導體基板 1‧‧‧Semiconductor substrate
10‧‧‧凹部 10‧‧‧recess
13‧‧‧第一摻雜區域 13‧‧‧First doped region
14‧‧‧第二摻雜區域 14‧‧‧Second doped region
D1‧‧‧距離 D1‧‧‧Distance
D2‧‧‧距離 D2‧‧‧Distance
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US5110755A (en) * | 1990-01-04 | 1992-05-05 | Westinghouse Electric Corp. | Process for forming a component insulator on a silicon substrate |
US20110081766A1 (en) * | 2009-10-02 | 2011-04-07 | Taiwan Semiconductor Manufacturing Company, Ltd. | Method for doping a selected portion of a device |
CN102569492A (en) * | 2010-12-17 | 2012-07-11 | 上海凯世通半导体有限公司 | Doping method for solar energy wafer and doped wafer |
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JP2002170963A (en) * | 2000-12-01 | 2002-06-14 | Sanken Electric Co Ltd | Semiconductor element, manufacturing method thereof and semiconductor device |
JP4631268B2 (en) * | 2003-10-29 | 2011-02-16 | 富士電機システムズ株式会社 | Semiconductor device |
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US8125056B2 (en) * | 2009-09-23 | 2012-02-28 | Vishay General Semiconductor, Llc | Double trench rectifier |
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US5110755A (en) * | 1990-01-04 | 1992-05-05 | Westinghouse Electric Corp. | Process for forming a component insulator on a silicon substrate |
US20110081766A1 (en) * | 2009-10-02 | 2011-04-07 | Taiwan Semiconductor Manufacturing Company, Ltd. | Method for doping a selected portion of a device |
CN102569492A (en) * | 2010-12-17 | 2012-07-11 | 上海凯世通半导体有限公司 | Doping method for solar energy wafer and doped wafer |
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