TW201905975A - Method of fabricating semiconductor device - Google Patents
Method of fabricating semiconductor deviceInfo
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- TW201905975A TW201905975A TW106121554A TW106121554A TW201905975A TW 201905975 A TW201905975 A TW 201905975A TW 106121554 A TW106121554 A TW 106121554A TW 106121554 A TW106121554 A TW 106121554A TW 201905975 A TW201905975 A TW 201905975A
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- photoresist layer
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 44
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 24
- 229920002120 photoresistant polymer Polymers 0.000 claims abstract description 52
- 239000000758 substrate Substances 0.000 claims abstract description 32
- 238000005468 ion implantation Methods 0.000 claims abstract description 15
- 238000000034 method Methods 0.000 claims abstract description 8
- 238000001459 lithography Methods 0.000 claims description 4
- 238000000206 photolithography Methods 0.000 abstract 1
- 239000000969 carrier Substances 0.000 description 5
- 230000015556 catabolic process Effects 0.000 description 4
- 230000005684 electric field Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 230000005676 thermoelectric effect Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 239000002784 hot electron Substances 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 229920005591 polysilicon Polymers 0.000 description 1
- 238000004904 shortening Methods 0.000 description 1
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Abstract
Description
本發明係有關於半導體裝置,特別是有關於輕摻雜汲極之半導體裝置之製造方法。 The present invention relates to semiconductor devices, and more particularly to a method of fabricating a lightly doped drain semiconductor device.
為了增加元件的密集度,提升運作的速度與效能,因此在半導體裝置的製程中,係持續地將元件的尺寸縮小。以MOS電晶體為例,由於通道長度的縮短以及閘極氧化層厚度的下降,使得垂直電場與水平電場增加。水平電場增加的結果,會加速通道中載子的速度,當這些載子在通道中加速獲得足夠的能量時,會增加這些載子注入到閘極氧化層中的機率,或是越過氧化層形成閘極電流,或者載子會在汲極端產生電子電洞對。所以當MOS電晶體的通道縮短,通道接近汲極的載子數量將上升而造成熱電子效應(Hot Electron Effect)。於熱電子效應中,部分電子射入閘極氧化層裡,所產生對應之電洞將流往基板(substrate)而產生基板電流。另一部分的電洞則被源極所收集,這使得NPN雙載子電晶體之現象加強,促使更多載子倍增,甚至可能進而發生電崩潰(Electrical Breakdown)情況。 In order to increase the density of components and improve the speed and performance of the operation, the size of the components is continuously reduced in the manufacturing process of the semiconductor device. Taking a MOS transistor as an example, the vertical electric field and the horizontal electric field are increased due to the shortening of the channel length and the decrease in the thickness of the gate oxide layer. As a result of the increase in the horizontal electric field, the velocity of the carriers in the channel is accelerated. When these carriers are accelerated in the channel to obtain sufficient energy, the probability of these carriers being injected into the gate oxide layer is increased, or the oxide layer is formed. The gate current, or the carrier, will create an electron hole pair at the 汲 extreme. Therefore, when the channel of the MOS transistor is shortened, the number of carriers whose channel is close to the drain will rise to cause a hot electron effect. In the hot electron effect, part of the electrons are injected into the gate oxide layer, and the corresponding holes are generated to flow to the substrate to generate the substrate current. The other part of the hole is collected by the source, which strengthens the phenomenon of the NPN bipolar transistor, which causes more carriers to multiply, and may even cause an electrical breakdown.
對於前述問題,習知的技術係提出輕摻雜汲極(Lightly Doped Drain,LDD)來減緩或避免熱電子效應對半導 體裝置所造成的損害。在半導體製程中,傳統的輕摻雜汲極的製造方法,仍有可以進一步改善之處;而本發明的用意是希望針對輕摻雜汲極提出新的半導體裝置之製造方法。 For the foregoing problems, the prior art has proposed a Lightly Doped Drain (LDD) to mitigate or avoid damage to the semiconductor device caused by the thermoelectric effect. In the semiconductor process, the conventional light-doped bungee manufacturing method can still be further improved; and the intention of the present invention is to propose a new semiconductor device manufacturing method for the lightly doped gate.
依據本發明之一技術特徵,本發明提出的一種半導體裝置之製造方法,至少包括如下的步驟。首先,形成一閘極結構於一半導體基板上。接著,形成一光阻層於該閘極結構上,該光阻層至少有一窄部分,且該窄部分的寬度小於該閘極的寬度,使得該閘極的一第一側部和一第二側部露出於該光阻層的兩側。然後進行離子佈植,以在該閘極結構兩側的該半導體基板中形成輕摻雜汲極區。 According to a technical feature of the present invention, a method of fabricating a semiconductor device according to the present invention includes at least the following steps. First, a gate structure is formed on a semiconductor substrate. Then, a photoresist layer is formed on the gate structure, the photoresist layer has at least a narrow portion, and the width of the narrow portion is smaller than the width of the gate, such that a first side portion and a second portion of the gate electrode The side portions are exposed on both sides of the photoresist layer. Ion implantation is then performed to form a lightly doped drain region in the semiconductor substrate on either side of the gate structure.
其中,分別露出於該光阻層的兩側的該第一側部和該第二側部具有實質上相等的寬度B。此外,該光阻層的該窄部分的寬度為S,該閘極結構的寬度為L,而且前述各個寬度L、B、S分別符合製程能力之規範。又,進行該離子佈植所使用的能量為100keV~200keV。 The first side portion and the second side portion respectively exposed on both sides of the photoresist layer have substantially equal widths B. Further, the narrow portion of the photoresist layer has a width S, the gate structure has a width L, and the respective widths L, B, and S respectively conform to the specifications of the process capability. Further, the energy used for the ion implantation is 100 keV to 200 keV.
依據本發明之另一技術特徵,本發明提出的一種半導體裝置之製造方法,至少包括如下步驟。首先,形成一閘極結構於一半導體基板上。再使用定義有兩個透光區的一遮罩,以微影製程形成具有兩個開口部的一光阻層於該半導體基板上;其中,該光阻層位於該兩個開口部之間的一第一光阻層係對準該閘極結構而形成於該閘極結構上、且該第一光阻層的寬度小於該閘極結構的寬度,使得該閘極結構的一第一側部和一第二側部露出於該第一光阻層的兩側。接著,進行離子佈 植,以在露出於該光阻層的該閘極結構兩側的該半導體基板中形成輕摻雜汲極區。 According to another technical feature of the present invention, a method of fabricating a semiconductor device according to the present invention includes at least the following steps. First, a gate structure is formed on a semiconductor substrate. And using a mask defined by two light-transmissive regions, forming a photoresist layer having two openings on the semiconductor substrate by a lithography process; wherein the photoresist layer is located between the two openings A first photoresist layer is formed on the gate structure in alignment with the gate structure, and a width of the first photoresist layer is smaller than a width of the gate structure, such that a first side of the gate structure And a second side portion is exposed on both sides of the first photoresist layer. Next, ion implantation is performed to form a lightly doped drain region in the semiconductor substrate exposed on both sides of the gate structure of the photoresist layer.
其中,分別露出於該第一光阻層的兩側的該第一側部和該第二側部具有實質上相等的寬度B。此外,該第一光阻層的寬度為S,該閘極結構的寬度為L,而且L、B、S分別符合製程能力之規範。又,進行該離子佈植所使用的能量為100keV~200keV。 The first side portion and the second side portion respectively exposed on both sides of the first photoresist layer have substantially equal widths B. In addition, the width of the first photoresist layer is S, the width of the gate structure is L, and L, B, and S respectively meet the specifications of the process capability. Further, the energy used for the ion implantation is 100 keV to 200 keV.
以下會依範例實施例並參照所附圖式,對本發明進行詳細的說明。 The present invention will now be described in detail by way of example embodiments with reference to the accompanying drawings.
10‧‧‧半導體基板 10‧‧‧Semiconductor substrate
12‧‧‧閘極結構 12‧‧‧ gate structure
12a‧‧‧閘極氧化層 12a‧‧‧ gate oxide layer
12b‧‧‧閘極 12b‧‧‧ gate
14‧‧‧光阻層 14‧‧‧ photoresist layer
16‧‧‧輕摻雜汲極區 16‧‧‧Lightly doped bungee zone
18‧‧‧離子佈植 18‧‧‧Ion implantation
20‧‧‧開口區 20‧‧‧Open area
31-34‧‧‧MOS電晶體特性曲線 31-34‧‧‧MOS transistor characteristic curve
40‧‧‧半導體基板 40‧‧‧Semiconductor substrate
42‧‧‧閘極結構 42‧‧‧ gate structure
42a‧‧‧閘極氧化層 42a‧‧‧ gate oxide layer
42b‧‧‧閘極 42b‧‧‧ gate
44‧‧‧光阻層 44‧‧‧ photoresist layer
44a‧‧‧第一光阻層 44a‧‧‧First photoresist layer
46‧‧‧輕摻雜汲極區 46‧‧‧Lightly doped bungee zone
48‧‧‧離子佈植 48‧‧‧Ion implantation
OP1-OP2‧‧‧開口部 OP1-OP2‧‧‧ openings
61-63‧‧‧MOS電晶體特性曲線 61-63‧‧‧MOS transistor characteristic curve
71-72‧‧‧MOS電晶體特性曲線 71-72‧‧‧MOS transistor characteristic curve
81-82‧‧‧MOS電晶體特性曲線 81-82‧‧‧MOS transistor characteristic curve
L‧‧‧閘極結構的寬度 L‧‧‧ width of gate structure
S‧‧‧第一光阻層的寬度 S‧‧‧The width of the first photoresist layer
B‧‧‧第一(第二)側部的寬度 B‧‧‧Width of the first (second) side
SP1‧‧‧第一側部 SP1‧‧‧ first side
SP2‧‧‧第二側部 SP2‧‧‧ second side
第1A~1C圖顯示習知輕摻雜汲極的製造流程。 Figures 1A to 1C show the manufacturing process of a conventional lightly doped drain.
第2圖顯示第1B圖的對應佈局圖。 Fig. 2 is a view showing a corresponding layout of Fig. 1B.
第3A~3B圖顯示以第2圖之佈局方式得到之MOS電晶體的電性特徵圖。 Figs. 3A to 3B are diagrams showing electrical characteristics of the MOS transistor obtained in the layout of Fig. 2.
第4A~4C圖顯示依據本發明實施例之輕摻雜汲極的製造流程。 4A-4C show a manufacturing process of a lightly doped drain according to an embodiment of the present invention.
第5圖顯示第4B圖對應的佈局圖。 Fig. 5 shows a layout corresponding to Fig. 4B.
第6圖顯示MOS電晶體的基板電流Isub相對於閘極電壓Vgate的特性圖。 Fig. 6 is a graph showing the characteristics of the substrate current Isub of the MOS transistor with respect to the gate voltage Vgate.
第7圖顯示MOS電晶體的汲極電流Idrain相對於汲極電壓Vdrain的特性圖。 Fig. 7 is a graph showing the characteristic of the drain current Idrain of the MOS transistor with respect to the gate voltage Vdrain.
第8圖顯示MOS電晶體的崩潰電壓特性圖。 Fig. 8 is a graph showing the breakdown voltage characteristics of the MOS transistor.
以下說明是本發明的各種實施範例及樣態。其目的是要舉例說明本發明一般性的原則,不應視為本發明之限制,本發明之範圍當以申請專利範圍所界定者為準。 The following description is of various embodiments and aspects of the invention. The intent is to exemplify the general principles of the invention and should not be construed as limiting the scope of the invention, which is defined by the scope of the claims.
第1A~1C圖顯示習知輕摻雜汲極(Lightly doped Drain,LDD)的製造流程。第1A圖中,形成一閘極結構12於一半導體基板10上,該半導體基板10例如是經過摻雜的矽(doped-silicon),該閘極結構12包括一閘極氧化層12a和例如經過摻雜的多晶閘極(doped-poly gate)12b,但是並非限定於此。第1B圖中,先利用光罩(未圖示)配合微影製程,形成一光阻層14於該半導體基板10上。第2圖顯示第1B圖的對應佈局圖。由第1B圖和第2圖可知,所使用的該光罩(未圖示)具有一透光區,以定義該光阻層14所具有的一開口區20(第2圖)。接著,進行離子佈植18以形成輕摻雜汲極區16,在去除該光阻層14之後則如第1C圖所示。 Figures 1A to 1C show the manufacturing process of a conventional Lightly doped Drain (LDD). In FIG. 1A, a gate structure 12 is formed on a semiconductor substrate 10, such as doped-silicon, which includes a gate oxide layer 12a and, for example, The doped-poly gate 12b is doped, but is not limited thereto. In Fig. 1B, a photomask layer 14 is formed on the semiconductor substrate 10 by a photomask (not shown) in cooperation with a lithography process. Fig. 2 is a view showing a corresponding layout of Fig. 1B. As can be seen from Figures 1B and 2, the photomask (not shown) used has a light transmissive region defining an open region 20 (Fig. 2) of the photoresist layer 14. Next, ion implantation 18 is performed to form lightly doped drain regions 16, which are shown in FIG. 1C after removal of the photoresist layer 14.
如上述習知的輕摻雜汲極的製造方法中,閘極結構12的大部分都露出於光阻層14的開口區20內,因此在進行高能量的離子佈植時,高能量離子容易從閘極結構12穿透至該半導體基板10,這會導致汲極至源極擊穿漏電(drain to source punch-through leakage)。此外,以第2圖所示的佈局結構為例,在中等電壓(5V~8V)的應用上,熱電子效應仍是非常嚴重。為了進一步降低熱電子效應,一般是將閘極結構12的寬度加大(也對應地加大了MOS電晶體的通道長度),以在高汲極電壓的場合中降低橫向電場。第3A圖中,曲線31表示閘極寬度L為0.8μm的MOS電晶體之特性,而曲線32表示閘極寬度L為0.85μm 的MOS電晶體之特性。如第3A圖所示,隨著閘極結構12的寬度L的增加,基板電流Isub則隨之減小。但是,隨著閘極結構12的寬度L的增加,會影響半導體裝置的尺寸,以及其電流驅動能力。第3B圖中,曲線33表示閘極寬度L為0.8μm的MOS電晶體之特性,而曲線34表示閘極寬度L為0.85μm的MOS電晶體之特性;如第3B圖所示,隨著閘極結構12的寬度L的增加,汲極電流Idrain也隨之減小。 In the above-described conventional method of manufacturing a lightly doped gate, most of the gate structure 12 is exposed in the open region 20 of the photoresist layer 14, so that high energy ions are easily used in high energy ion implantation. Penetration from the gate structure 12 to the semiconductor substrate 10 results in drain to source punch-through leakage. In addition, taking the layout structure shown in Fig. 2 as an example, the thermoelectric effect is still very serious in medium voltage (5V~8V) applications. In order to further reduce the thermoelectric effect, the width of the gate structure 12 is generally increased (and the channel length of the MOS transistor is correspondingly increased) to reduce the lateral electric field in the case of a high drain voltage. In Fig. 3A, a curve 31 indicates characteristics of a MOS transistor having a gate width L of 0.8 μm, and a curve 32 indicates characteristics of a MOS transistor having a gate width L of 0.85 μm. As shown in FIG. 3A, as the width L of the gate structure 12 increases, the substrate current Isub decreases. However, as the width L of the gate structure 12 increases, the size of the semiconductor device and its current driving capability are affected. In Fig. 3B, curve 33 represents the characteristics of the MOS transistor having a gate width L of 0.8 μm, and curve 34 represents the characteristics of the MOS transistor having a gate width L of 0.85 μm; as shown in Fig. 3B, with the gate As the width L of the pole structure 12 increases, the drain current Idrain also decreases.
第4A~4C圖顯示依據本發明實施例之輕摻雜汲極的製造流程。第5圖顯示第4B圖對應的佈局圖。 4A-4C show a manufacturing process of a lightly doped drain according to an embodiment of the present invention. Fig. 5 shows a layout corresponding to Fig. 4B.
第4A圖中,形成一閘極結構42於一半導體基板40上,該半導體基板40例如是經過摻雜的矽基板(doped-silicon substrate),該閘極結構42包括一閘極氧化層42a和例如經過摻雜的多晶矽閘極(doped-poly gate)42b,但是並非限定於此。 In FIG. 4A, a gate structure 42 is formed on a semiconductor substrate 40, such as a doped-silicon substrate, the gate structure 42 includes a gate oxide layer 42a and For example, the doped polysilicon gate 42b is doped, but is not limited thereto.
第4B圖中,使用定義有兩個透光區的一遮罩(未圖示),以微影製程形成具有兩個開口部OP1、OP2(第5圖)的一光阻層44於該半導體基板40上。其中,該光阻層42位於該兩個開口部OP1、OP2之間的一第一光阻層44a係對準該閘極結構42、且該第一光阻層44a的寬度S小於該閘極結構42的寬度L,使得該閘極結構42的一第一側部SP1和一第二側部SP2露出於該第一光阻層44a的兩側。 In FIG. 4B, a mask (not shown) defining two light-transmissive regions is used to form a photoresist layer 44 having two openings OP1, OP2 (Fig. 5) in the lithography process. On the substrate 40. The first photoresist layer 44a of the photoresist layer 42 between the two openings OP1 and OP2 is aligned with the gate structure 42 and the width S of the first photoresist layer 44a is smaller than the gate. The width L of the structure 42 is such that a first side portion SP1 and a second side portion SP2 of the gate structure 42 are exposed on both sides of the first photoresist layer 44a.
接著,進行離子佈植48,以在露出於該光阻層44的該閘極結構42兩側的該半導體基板40中形成輕摻雜汲極區46,在去除該光阻層44後,如第4C圖所示。在此,進行輕摻雜汲極之離子佈植所使用的能量可以是100keV~200keV。 Next, ion implantation 48 is performed to form a lightly doped drain region 46 in the semiconductor substrate 40 exposed on both sides of the gate structure 42 of the photoresist layer 44. After removing the photoresist layer 44, Figure 4C shows. Here, the energy used for ion implantation of the lightly doped drain may be 100 keV to 200 keV.
請參照第5圖,該閘極結構42的寬度為L、該第一光阻層44a的寬度為S,於本發明的範例中寬度S和寬度L的比例(S/L)為3/4~5/8;例如,S/L一般可為0.6μm/0.8μm、較佳的為0.55μm/0.8μm、更佳的為0.5μm/0.8μm。此外,該閘極結構42露出於該第一光阻層44a兩側的該第一側部SP1和該第二側部SP2的可以是相等的寬度B、但亦可以不同寬度。寬度B亦即是第一光阻層44a的邊緣與該閘極結構42的邊緣的距離。又,寬度S大於寬度B,又當第一側部SP1和該第二側部SP2具有相等的寬度B時,L=S+2B。 Referring to FIG. 5, the width of the gate structure 42 is L, the width of the first photoresist layer 44a is S, and the ratio of the width S to the width L (S/L) is 3/4 in the example of the present invention. ~5/8; For example, S/L may generally be 0.6 μm / 0.8 μm, preferably 0.55 μm / 0.8 μm, more preferably 0.5 μm / 0.8 μm. In addition, the first side portion SP1 and the second side portion SP2 of the gate structure 42 exposed on both sides of the first photoresist layer 44a may have the same width B, but may have different widths. The width B is also the distance between the edge of the first photoresist layer 44a and the edge of the gate structure 42. Further, the width S is larger than the width B, and when the first side portion SP1 and the second side portion SP2 have the same width B, L = S + 2B.
第6~8圖顯示應用本發明半導體裝置之製造方法所得到的具有輕摻雜汲極的MOS電晶體的電性特徵圖。 6 to 8 are views showing electrical characteristics of a MOS transistor having a lightly doped drain obtained by applying the manufacturing method of the semiconductor device of the present invention.
第6圖顯示MOS電晶體的基板電流Isub相對於閘極電壓Vgate的特性圖。第6圖中,曲線61、62所對應的MOS電晶體的輕摻雜汲極係以第2圖的佈局方式所形成、且其閘極結構的寬度分別為0.8μm和0.85μm;曲線63所對應的MOS電晶體的輕摻雜汲極係以本發明揭示之第5圖的佈局方式所形成、且其閘極結構的寬度為0.8μm。由第6圖明顯可知,應用本發明可以將基板電流|Isub|的頂點值由曲線61的約52μA/μm降低至約36μA/μm。值得注意的是,即使曲線63的MOS電晶體沒有增加閘極結構的寬度L(0.8μm),但是其降低基板電流Isub的效能表現更優於曲線62的MOS電晶體(寬度L增為0.85μm)。 Fig. 6 is a graph showing the characteristics of the substrate current Isub of the MOS transistor with respect to the gate voltage Vgate. In Fig. 6, the lightly doped gates of the MOS transistors corresponding to the curves 61 and 62 are formed in the layout of Fig. 2, and the widths of the gate structures are 0.8 μm and 0.85 μm, respectively; The lightly doped gate of the corresponding MOS transistor is formed in the layout of the fifth embodiment of the present invention, and the width of the gate structure is 0.8 μm. As is apparent from Fig. 6, the apex value of the substrate current |Isub| can be lowered from about 52 μA/μm of the curve 61 to about 36 μA/μm by applying the present invention. It is worth noting that even if the MOS transistor of the curve 63 does not increase the width L (0.8 μm) of the gate structure, its performance of lowering the substrate current Isub is better than that of the MOS transistor of the curve 62 (the width L is increased to 0.85 μm). ).
第7圖顯示MOS電晶體的汲極電流Idrain相對於汲極電壓Vdrain的特性圖。第7圖中,曲線71所對應的MOS電晶體的輕摻雜汲極係以第2圖的佈局方式所形成、且其閘極結構 的寬度為0.8μm;曲線72所對應的MOS電晶體的輕摻雜汲極係以本發明揭示之第5圖的佈局方式所形成、且其閘極結構的寬度為0.8μm。由第7圖的結果可知,曲線72所對應的MOS電晶體的汲極電流Idrain均大於曲線71所對應的MOS電晶體的汲極電流,亦即曲線72的MOS電晶體的電流驅動能力優於曲線71的MOS電晶體的電流驅動能力。因此,應用本發明,不會減損MOS電晶體的電流驅動能力。 Fig. 7 is a graph showing the characteristic of the drain current Idrain of the MOS transistor with respect to the gate voltage Vdrain. In Fig. 7, the lightly doped gate of the MOS transistor corresponding to the curve 71 is formed in the layout of Fig. 2, and the width of the gate structure is 0.8 μm; the MOS transistor corresponding to the curve 72 The lightly doped drain is formed by the layout of the fifth embodiment of the present invention, and the width of the gate structure is 0.8 μm. It can be seen from the results of FIG. 7 that the drain current Idrain of the MOS transistor corresponding to the curve 72 is larger than the drain current of the MOS transistor corresponding to the curve 71, that is, the current driving capability of the MOS transistor of the curve 72 is better. The current drive capability of the MOS transistor of curve 71. Therefore, the application of the present invention does not detract from the current drive capability of the MOS transistor.
第8圖顯示MOS電晶體的崩潰電壓特性圖。第8圖中,曲線81所對應的MOS電晶體的輕摻雜汲極係以第2圖的佈局方式所形成、且其閘極結構的寬度為0.8μm;曲線82所對應的MOS電晶體的輕摻雜汲極係以本發明揭示之第5圖的佈局方式所形成、且其閘極結構的寬度為0.8μm。第8圖的橫軸代表汲極電壓Vdrain,而縱軸代表取對數值的汲極漏電流log(Idrain)。由第8圖的結果明顯可知,應用本發明並不會對MOS電晶體的崩潰特性造成損害。 Fig. 8 is a graph showing the breakdown voltage characteristics of the MOS transistor. In Fig. 8, the lightly doped gate of the MOS transistor corresponding to the curve 81 is formed in the layout of Fig. 2, and the width of the gate structure is 0.8 μm; the MOS transistor corresponding to the curve 82 The lightly doped drain is formed by the layout of the fifth embodiment of the present invention, and the width of the gate structure is 0.8 μm. The horizontal axis of Fig. 8 represents the drain voltage Vdrain, and the vertical axis represents the logarithmic drain leakage current log (Idrain). As is apparent from the results of Fig. 8, the application of the present invention does not impair the collapse characteristics of the MOS transistor.
以第2圖所示的佈局方式,係以單一開口(20)對半導體基板進行製造輕摻雜汲極的離子佈植;而本發明以第5圖所示的佈局方式,係以二個開口部(SP1、SP2)對半導體基板進行製造輕摻雜汲極的離子佈植,即能在有效地降低基板電流,無需增加閘極結構的寬度L進而避免降低MOS電晶體的電流驅動能力。此外,亦不會對MOS電晶體的崩潰特性造成影響。 In the layout shown in FIG. 2, the semiconductor substrate is ion-implanted with a single opening (20) to fabricate a lightly doped drain; and the present invention has two openings in the layout shown in FIG. The parts (SP1, SP2) fabricate the light-doped drain of the semiconductor substrate, which can effectively reduce the substrate current without increasing the width L of the gate structure and avoid reducing the current driving capability of the MOS transistor. In addition, it does not affect the breakdown characteristics of MOS transistors.
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