TWI713096B - Method of fabricating semiconductor device - Google Patents

Method of fabricating semiconductor device Download PDF

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TWI713096B
TWI713096B TW106121554A TW106121554A TWI713096B TW I713096 B TWI713096 B TW I713096B TW 106121554 A TW106121554 A TW 106121554A TW 106121554 A TW106121554 A TW 106121554A TW I713096 B TWI713096 B TW I713096B
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photoresist layer
gate structure
width
gate
semiconductor manufacturing
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TW201905975A (en
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林志威
林宗漢
吳昭緯
陳彥凱
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世界先進積體電路股份有限公司
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Abstract

A method of fabricating a semiconductor device includes the following steps. First, form a gate structure on a semiconductor substrate. Then, use a mask having two transparent regions through a photolithography process to form a photoresist layer having two openings in the semiconductor substrate. A first photoresist layer of the photoresist layer between the two openings is aligned to the gate structure and formed on the gate structure. The width of the first photoresist layer is smaller than that of the gate structure such that a first side portion and a second side portion of the gate structure are not covered by the first photoresist layer. Next, carry out ion implantation to form lightly doped drain regions in the semiconductor substrate which are not covered by the photoresist layer.

Description

半導體裝置之製造方法 Manufacturing method of semiconductor device

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, in particular to methods for manufacturing lightly doped drain semiconductor devices.

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 increase the speed and performance of operation, the size of components is continuously reduced in the manufacturing process of semiconductor devices. Taking the MOS transistor as an example, the vertical electric field and the horizontal electric field increase due to the shortening of the channel length and the decrease of the thickness of the gate oxide layer. As a result of the increase in the horizontal electric field, the speed of carriers in the channel will be accelerated. When these carriers accelerate in the channel to obtain sufficient energy, the probability of these carriers being injected into the gate oxide layer or formed across the oxide layer The gate current, or carrier will generate electron hole pairs at the drain terminal. Therefore, when the channel of the MOS transistor is shortened, the number of carriers close to the drain of the channel will increase and cause the hot electron effect (Hot Electron Effect). In the hot electron effect, part of the electrons are injected into the gate oxide layer, and the corresponding holes generated will flow to the substrate to generate a substrate current. The other part of the holes is collected by the source, which strengthens the phenomenon of the NPN bi-carrier transistor, prompting more carriers to multiply, and even electrical breakdown (Electrical Breakdown) may occur.

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。 Regarding the aforementioned problems, the conventional technology proposes a lightly doped drain (LDD) to slow down or avoid damage to the semiconductor device caused by the hot electron effect. In the semiconductor manufacturing process, the traditional lightly doped drain manufacturing method can still be further improved; and the intention of the present invention is to propose a new manufacturing method for the lightly doped drain.

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 one of the technical features of the present invention, a method of manufacturing a semiconductor device proposed by 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, so that a first side portion and a second side of the gate are The side portions are exposed on both sides of the photoresist layer. Then ion implantation is performed to form lightly doped drain regions in the semiconductor substrate on both sides 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。 Wherein, the first side portion and the second side portion respectively exposed on both sides of the photoresist layer have substantially the same width B. In addition, the width of the narrow portion of the photoresist layer is S, the width of the gate structure is L, and the aforementioned respective widths L, B, and S meet the specifications of process capability. In addition, the energy used to perform this 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 manufacturing a semiconductor device provided by the present invention includes at least the following steps. First, a gate structure is formed on a semiconductor substrate. Using a mask defined with two light-transmitting areas, a photoresist layer with two openings is formed on the semiconductor substrate by a photolithography process; wherein, the photoresist layer is located between the two openings. A first photoresist layer is formed on the gate structure by aligning with the gate structure, and the width of the first photoresist layer is smaller than the width of the gate structure, so that a first side portion 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 lightly doped drain regions 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。 Wherein, the first side portion and the second side portion respectively exposed on both sides of the first photoresist layer have substantially the same width 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 meet the specifications of process capability respectively. In addition, the energy used to perform this 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。 Hereinafter, the present invention will be described in detail based on exemplary embodiments and 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

12b‧‧‧閘極 12b‧‧‧Gate

14‧‧‧光阻層 14‧‧‧Photoresist layer

16‧‧‧輕摻雜汲極區 16‧‧‧Lightly doped drain region

18‧‧‧離子佈植 18‧‧‧Ion implantation

20‧‧‧開口區 20‧‧‧Opening 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

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 drain region

48‧‧‧離子佈植 48‧‧‧Ion implantation

OP1-OP2‧‧‧開口部 OP1-OP2‧‧‧Opening

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‧‧‧The width of the 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‧‧‧The 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~1C show the manufacturing process of the conventional lightly doped drain.

第2圖顯示第1B圖的對應佈局圖。 Figure 2 shows the corresponding layout of Figure 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。 Figures 3A~3B show the electrical characteristics of the MOS transistor obtained by the layout of Figure 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 to 4C show the manufacturing process of the 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。 Figure 5 shows the layout corresponding to Figure 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。 Figure 6 shows the characteristic diagram 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。 Figure 7 shows the characteristic diagram of the drain current Idrain of the MOS transistor with respect to the drain voltage Vdrain.

第8圖顯示MOS電晶體的崩潰電壓特性圖。 Figure 8 shows the breakdown voltage characteristics of MOS transistors.

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 descriptions are various implementation examples and aspects of the present invention. Its purpose is to exemplify the general principles of the present invention, and should not be regarded as a limitation of the present invention. The scope of the present invention should be defined by the scope of the patent application.

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~1C show the manufacturing process of the conventional lightly doped drain (LDD). In Figure 1A, a gate structure 12 is formed on a semiconductor substrate 10. The semiconductor substrate 10 is, for example, doped-silicon. The gate structure 12 includes a gate oxide layer 12a and The doped-poly gate 12b is not limited to this. In FIG. 1B, a photoresist layer 14 is formed on the semiconductor substrate 10 by using a photomask (not shown) in conjunction with a lithography process. Figure 2 shows the corresponding layout of Figure 1B. It can be seen from FIG. 1B and FIG. 2 that the used photomask (not shown) has a light-transmitting area to define an opening area 20 of the photoresist layer 14 (FIG. 2). Next, ion implantation 18 is performed to form the lightly doped drain region 16, as shown in FIG. 1C after the photoresist layer 14 is removed.

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。 As in the above-mentioned conventional lightly doped drain manufacturing method, most of the gate structure 12 is exposed in the opening area 20 of the photoresist layer 14. Therefore, high-energy ions are easily implanted during high-energy ion implantation. The penetration from the gate structure 12 to the semiconductor substrate 10 will cause drain to source punch-through leakage. In addition, taking the layout structure shown in Figure 2 as an example, the hot electron effect is still very serious in the application of medium voltage (5V~8V). In order to further reduce the hot electron 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 occasion of high drain voltage. In Fig. 3A, curve 31 represents the characteristics of a MOS transistor with a gate width L of 0.8 μm, and curve 32 represents the characteristics of a MOS transistor with 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 accordingly. However, as the width L of the gate structure 12 increases, the size of the semiconductor device and its current driving capability will be affected. In Figure 3B, curve 33 shows the characteristics of a MOS transistor with a gate width L of 0.8μm, and curve 34 shows the characteristics of a MOS transistor with a gate width L of 0.85μm; as shown in Figure 3B, as 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 to 4C show the manufacturing process of the lightly doped drain according to an embodiment of the present invention. Figure 5 shows the layout corresponding to Figure 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. The semiconductor substrate 40 is, for example, a doped-silicon substrate. The gate structure 42 includes a gate oxide layer 42a and For example, a doped-poly gate 42b is doped, but it is not limited to this.

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 Figure 4B, a mask (not shown) defining two light-transmitting regions is used to form a photoresist layer 44 with two openings OP1 and OP2 (Figure 5) on the semiconductor by a photolithography process. On the substrate 40. Wherein, a first photoresist layer 44a of the photoresist layer 42 located 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 makes a first side SP1 and a second side SP2 of the gate structure 42 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 lightly doped drain regions 46 in the semiconductor substrate 40 exposed on both sides of the gate structure 42 of the photoresist layer 44. After the photoresist layer 44 is removed, such as As shown in Figure 4C. Here, the energy used for ion implantation of lightly doped drain can be 100keV~200keV.

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 and the width of the first photoresist layer 44a is S. In the example of the present invention, the ratio (S/L) of the width S to the width L is 3/4 ~5/8; For example, S/L can generally be 0.6μm/0.8μm, preferably 0.55μm/0.8μm, more preferably 0.5μm/0.8μm. In addition, the gate structure 42 exposed on both sides of the first photoresist layer 44a may have the same width B of the first side portion SP1 and the second side portion SP2, but may also have different widths. The width B is the distance between the edge of the first photoresist layer 44a and the edge of the gate structure 42. Moreover, the width S is greater 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。 Figures 6 to 8 show electrical characteristic diagrams of MOS transistors with lightly doped drains obtained by applying the semiconductor device manufacturing method 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)。 Figure 6 shows the characteristic diagram of the substrate current Isub of the MOS transistor with respect to the gate voltage Vgate. In Figure 6, the lightly doped drains of the MOS transistors corresponding to curves 61 and 62 are formed in the layout of Figure 2, and the widths of their gate structures are 0.8 μm and 0.85 μm, respectively; as shown in curve 63 The lightly doped drain of the corresponding MOS transistor is formed by the layout of FIG. 5 disclosed in the present invention, and the width of the gate structure is 0.8 μm. It is obvious from Fig. 6 that the application of the present invention can reduce the peak value of the substrate current |Isub| from about 52 μA/μm of the curve 61 to about 36 μA/μm. It is worth noting that even though the MOS transistor of curve 63 does not increase the width L (0.8 μm) of the gate structure, its performance in reducing the substrate current Isub is better than that of the MOS transistor of 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。 Figure 7 shows the characteristic diagram of the drain current Idrain of the MOS transistor with respect to the drain voltage Vdrain. In Figure 7, the lightly doped drain of the MOS transistor corresponding to curve 71 is formed in the layout of Figure 2, and the width of its gate structure is 0.8μm; the lightly doped drain of the MOS transistor corresponding to curve 72 is The lightly doped drain is formed by the layout of Figure 5 disclosed in the present invention, and the width of the gate structure is 0.8 μm. From the results in Figure 7, it can be seen that the drain current Idrain of the MOS transistor corresponding to curve 72 is greater than the drain current of the MOS transistor corresponding to curve 71, that is, the current drive capability of the MOS transistor of curve 72 is better than The current drive capability of the MOS transistor in curve 71. Therefore, the application of the present invention will not impair 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。 Figure 8 shows the breakdown voltage characteristics of MOS transistors. In Figure 8, the lightly doped drain of the MOS transistor corresponding to curve 81 is formed in the layout of Figure 2, and the width of its gate structure is 0.8 μm; the MOS transistor corresponding to curve 82 The lightly doped drain is formed by the layout of Figure 5 disclosed in the present invention, and the width of the gate structure is 0.8 μm. The horizontal axis of Figure 8 represents the drain voltage Vdrain, and the vertical axis represents the drain leakage current log(Idrain), which is a logarithmic value. It is obvious from the results in Fig. 8 that the application of the present invention will not damage the breakdown 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 Figure 2, a single opening (20) is used to fabricate lightly doped drain ion implantation on the semiconductor substrate; while the present invention uses the layout shown in Figure 5 to use two openings The parts (SP1, SP2) implant the lightly doped drain on the semiconductor substrate, which can effectively reduce the substrate current without increasing the width L of the gate structure to avoid reducing the current driving capability of the MOS transistor. In addition, it will not affect the breakdown characteristics of the MOS transistor.

42‧‧‧閘極結構 42‧‧‧Gate structure

44‧‧‧光阻層 44‧‧‧Photoresist layer

44a‧‧‧第一光阻層 44a‧‧‧First photoresist layer

OP1-OP2‧‧‧開口部 OP1-OP2‧‧‧Opening

L‧‧‧閘極結構的寬度 L‧‧‧The width of the 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‧‧‧The width of the first (second) side

SP1‧‧‧第一側部 SP1‧‧‧First side

SP2‧‧‧第二側部 SP2‧‧‧Second side

Claims (10)

一種半導體製造方法,包括:形成一閘極結構於一半導體基板上,其中該閘極結構包括一多晶矽閘極以及形成在該多晶矽閘極下的一閘極氧化層;形成一光阻層於該閘極結構的該多晶矽閘極上,其中該光阻層的寬度小於該閘極結構的寬度,使得該閘極結構的該多晶矽閘極是部分地接觸該光阻層且該閘極氧化層的一第一側部和一第二側部露出於該光阻層的兩側;以及在該閘極結構的寬度大於該光阻層的寬度時進行離子佈植,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,並去除該光阻層。 A semiconductor manufacturing method includes: forming a gate structure on a semiconductor substrate, wherein the gate structure includes a polysilicon gate and a gate oxide layer formed under the polysilicon gate; forming a photoresist layer on the On the polysilicon gate of the gate structure, wherein the width of the photoresist layer is smaller than the width of the gate structure, so that the polysilicon gate of the gate structure partially contacts the photoresist layer and a part of the gate oxide layer The first side portion and the second side portion are exposed on both sides of the photoresist layer; and ion implantation is performed when the width of the gate structure is greater than the width of the photoresist layer, so as to be on both sides of the gate structure A lightly doped drain region is formed in the semiconductor substrate, and the photoresist layer is removed. 如申請專利範圍第1項所述之半導體製造方法,其中該光阻層的寬度為S,該閘極結構的寬度為L,該光阻層的邊緣與該閘極結構的邊緣的距離為B,而且S>B。 The semiconductor manufacturing method as described in item 1 of the scope of patent application, wherein the width of the photoresist layer is S, the width of the gate structure is L, and the distance between the edge of the photoresist layer and the edge of the gate structure is B , And S>B. 如申請專利範圍第1項所述之半導體製造方法,其中分別露出於該光阻層的兩側的該閘極氧化層的該第一側部和該第二側部具有實質上相等的寬度B。 The semiconductor manufacturing method described in claim 1, wherein the first side portion and the second side portion of the gate oxide layer exposed on both sides of the photoresist layer respectively have substantially equal width B . 如申請專利範圍第3項所述之半導體製造方法,其中該光阻層的寬度為S,該閘極結構的寬度為L,而且L、B、S分別符合L=S+2B,S>B。 As for the semiconductor manufacturing method described in item 3 of the scope of patent application, the width of the photoresist layer is S, the width of the gate structure is L, and L, B, and S respectively meet L=S+2B, S>B . 如申請專利範圍第1項所述之半導體製造方法,其中進行該離子佈植所使用的能量為100keV~200keV。 The semiconductor manufacturing method described in the first item of the scope of patent application, wherein the energy used for the ion implantation is 100keV~200keV. 一種半導體製造方法,包括:形成一閘極結構於一半導體基板上,其中該閘極結構包括一 多晶矽閘極以及形成在該多晶矽閘極下的一閘極氧化層;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並部分地接觸於該閘極結構的該多晶矽閘極上、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;以及在該閘極的寬度大於該光阻層之該第一光阻層的寬度時進行離子佈植,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,並去除該光阻層。 A semiconductor manufacturing method includes: forming a gate structure on a semiconductor substrate, wherein the gate structure includes a Polysilicon gate and a gate oxide layer formed under the polysilicon gate; using a mask that defines two light-transmitting regions, a photoresist layer with two openings is formed on the semiconductor substrate by a photolithography process On; wherein, a first photoresist layer of the photoresist layer located between the two openings is aligned with the gate structure to form and partially contact the polysilicon gate of the gate structure, and the first The width of a photoresist layer is smaller than the width of the gate structure, so that a first side and a second side of the gate structure are exposed on both sides of the first photoresist layer; and at the width of the gate When the width of the first photoresist layer is larger than the photoresist layer, ion implantation is performed to form lightly doped drain regions in the semiconductor substrate exposed on both sides of the gate structure of the photoresist layer, and remove The photoresist layer. 如申請專利範圍第6項所述之半導體製造方法,其中該第一光阻層的寬度為S,該閘極結構的寬度為L,該第一光阻層的邊緣與該閘極結構的邊緣的距離為B,而且S>B。 The semiconductor manufacturing method described in item 6 of the scope of patent application, wherein the width of the first photoresist layer is S, the width of the gate structure is L, the edge of the first photoresist layer and the edge of the gate structure The distance is B, and S>B. 如申請專利範圍第6項所述之半導體製造方法,其中分別露出於該第一光阻層的兩側的該閘極氧化層的該第一側部和該第二側部具有實質上相等的寬度B。 According to the semiconductor manufacturing method described in claim 6, wherein the first side portion and the second side portion of the gate oxide layer exposed on both sides of the first photoresist layer have substantially equal Width B. 如申請專利範圍第8項所述之半導體製造方法,其中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L=S+2B,S>B。 The semiconductor manufacturing method described in item 8 of the scope of patent application, wherein the width of the first photoresist layer is S, the width of the gate structure is L, and L, B, and S meet L=S+2B, S >B. 如申請專利範圍第6項所述之半導體製造方法,其中進行該離子佈植所使用的能量為100keV~200keV。 The semiconductor manufacturing method described in item 6 of the scope of patent application, wherein the energy used for the ion implantation is 100keV~200keV.
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