TW201626464A - Field-effect transistor - Google Patents

Field-effect transistor Download PDF

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TW201626464A
TW201626464A TW104133519A TW104133519A TW201626464A TW 201626464 A TW201626464 A TW 201626464A TW 104133519 A TW104133519 A TW 104133519A TW 104133519 A TW104133519 A TW 104133519A TW 201626464 A TW201626464 A TW 201626464A
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effect transistor
field effect
mask layer
channel
region
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TW104133519A
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Chinese (zh)
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Masashi Uematsu
Kohei Itoh
Nobuya Mori
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Japan Science & Tech Agency
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor 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
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/78Field effect transistors with field effect produced by an insulated gate
    • H01L29/786Thin film transistors, i.e. transistors with a channel being at least partly a thin film

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  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Physics & Mathematics (AREA)
  • Ceramic Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Thin Film Transistor (AREA)

Abstract

A field-effect transistor (100) is provided with a channel (30c) formed of a semiconductor nano wire (30). A source region (30s) and a drain region (30d) are formed adjacent to the channel (30c), and a gate electrode (40) is provided above the channel. On the main surface of the semiconductor nano wire (30), a mask layer (50) is provided, said mask layer containing dopant atoms to be a donor or an acceptor. Though the dopant atoms are ion-implanted into the mask layer (50) on a side wall portion of the gate electrode (40) as well, the implanted ions stay at an upper portion, and are not implanted as far as to a portion in contact with the main surface of the semiconductor nano wire (30). Consequently, a mask layer portion formed with a thickness W on the side wall of the gate electrode (40) does not function as a diffusion source of the dopant.

Description

場效電晶體 Field effect transistor

本發明係關於具備有由半導體奈米線般之半導體材料部所形成之通道的場效電晶體,詳言之,係關於具有可抑制閾值電壓之偏差,同時可充分取得導通電流(ON current)之源極-汲極構造的場效電晶體。 The present invention relates to a field effect transistor having a channel formed by a semiconductor material portion such as a semiconductor nanowire, and more specifically, has a variation in suppressing a threshold voltage and can sufficiently obtain an ON current. The field-effect transistor of the source-dippole structure.

於形成使用半導體奈米線般之半導體材料部的場效電晶體時,係有必要針對源極區域及汲極區域進行摻雜,當將閘極電極當作遮罩而直接將摻雜物予以離子注入時,即便是進行熱處理,仍會有離子注入所造成之結晶缺陷殘留在電晶體本體上。 When forming a field effect transistor using a semiconductor nanowire-like semiconductor material portion, it is necessary to dope the source region and the drain region, and directly apply the dopant to the gate electrode as a mask. At the time of ion implantation, even if heat treatment is performed, crystal defects caused by ion implantation remain on the transistor body.

在利用固相擴散法進行摻雜而形成源極區域及汲極區域時,雖可避免如上所述之缺陷殘留,但會因為擴散而摻雜物侵入到通道區域,而有電晶體之閾值電壓偏移的問題。又,在為了抑制閾值電壓偏移而降低摻雜物濃度時,會變得無法取得充分的導通電流。 When the source region and the drain region are formed by doping by the solid phase diffusion method, the defect remaining as described above can be avoided, but the dopant invades into the channel region due to diffusion, and the threshold voltage of the transistor is present. The problem of offset. Further, when the dopant concentration is lowered to suppress the threshold voltage shift, a sufficient on-current cannot be obtained.

本發明者等係以抑制場效電晶體之閾值偏差為目的,而已檢討過如下技術:在將摻雜物予以離子注入前,先設置間隔體於閘極電極之側壁上,以使摻雜物不會注入到該側壁間隔體正下方之半導體區域(植松等 :非專利文獻1)。依此,藉由設置此類側壁間隔體,則摻雜物難以侵入至通道區域,其結果係可確認到能顯著抑制關閉電流(OFF current)之變動與閾值電壓之偏差。 The present inventors have aimed to suppress the threshold deviation of the field effect transistor, and have reviewed a technique of disposing a spacer on the sidewall of the gate electrode to ionize the dopant before ion implantation. Will not be implanted into the semiconductor region directly under the sidewall spacer (Uzun, etc.) : Non-Patent Document 1). As a result, by providing such a sidewall spacer, it is difficult for the dopant to intrude into the channel region, and as a result, it can be confirmed that the variation between the OFF current and the threshold voltage can be remarkably suppressed.

[先前技術文獻] [Previous Technical Literature] [非專利文獻] [Non-patent literature]

[非專利文獻1]M. Uematsu et al.,"Simulation of the Effect of Arsenic Discrete Distribution on Device Characteristics in Silicon Nanowire Transistors" IEDM12-709(2012) [Non-Patent Document 1] M. Uematsu et al., "Simulation of the Effect of Arsenic Discrete Distribution on Device Characteristics in Silicon Nanowire Transistors" IEDM12-709 (2012)

然而,即便如非專利文獻1所揭示般,在閘極電極側壁上設置間隔體,也無法充分抑制伴隨著離子注入後之熱處理等所造成之摻雜物朝向通道區域的侵入。況且,由於自摻雜物會有電子的「流出」,所以對於通道的影響,不僅是上述摻雜物的侵入,還需要考慮到該電子的「流出長度」。例如,在半導體奈米線為矽結晶,而摻雜物為砷時,電子的「流出長度」為2nm左右。 However, even if a spacer is provided on the sidewall of the gate electrode as disclosed in Non-Patent Document 1, it is not possible to sufficiently suppress the intrusion of the dopant into the channel region due to heat treatment or the like after ion implantation. Moreover, since the self-dopant has an "outflow" of electrons, the influence on the channel is not only the intrusion of the above dopant but also the "outflow length" of the electron. For example, when the semiconductor nanowire is germanium crystal and the dopant is arsenic, the "outflow length" of electrons is about 2 nm.

再者,即便有此類摻雜物的侵入和電子的「流出」,當於閘極長度較長的情況下,並不至於成為問題。惟,伴隨著場效電晶體的細微化,當閘極長度變短時,該摻雜物的侵入和電子的「流出」會大大地影響到通道區域,而導致閾值電壓之偏差的結果。因此,要求在更進一步抑制摻雜物對於通道區域之侵入的同時,還 考慮到電子的「流出長度」的通道形成技術(源極/汲極之形成技術)。又,亦有需要避開離子注入所造成之結晶缺陷會殘留於電晶體本體上的問題。 Furthermore, even if there is such an intrusion of such a dopant and an "outflow" of electrons, it does not become a problem when the gate length is long. However, with the miniaturization of the field effect transistor, when the gate length becomes shorter, the intrusion of the dopant and the "outflow" of the electron greatly affect the channel region, resulting in a deviation of the threshold voltage. Therefore, it is required to further suppress the intrusion of the dopant into the channel region while further suppressing A channel forming technique (source/drain formation technique) that takes into account the "outflow length" of electrons. Further, there is a need to avoid the problem that crystal defects caused by ion implantation remain on the transistor body.

本發明係有鑑於上述問題而完成者,其目的係在於提供一種具有可抑制閾值電壓偏差,同時能充分取得導通電流之源極-汲極構造,而且不會引起因離子注入至電晶體本體上所造成之結晶缺陷,具備由半導體奈米線般之半導體材料部所形成之通道的場效電晶體。 The present invention has been made in view of the above problems, and an object thereof is to provide a source-drain structure capable of suppressing a threshold voltage deviation while sufficiently obtaining an on-current, without causing ion implantation onto a transistor body. The resulting crystal defect is a field effect transistor having a channel formed by a semiconductor material portion of a semiconductor nanowire.

為了解決上述課題,本發明之第1態樣的場效電晶體之特徵為:其係具備有由厚度H(nm)之半導體材料部所形成的通道、鄰接該通道所形成的源極區域及汲極區域、設置在該通道上方的閘極區域之場效電晶體,其中該閘極區域之閘極長度(Lg)為4nm以上10nm以下,該通道之中央區域的摻雜原子數為1以下。 In order to solve the above problems, a field effect transistor according to a first aspect of the present invention is characterized in that it has a channel formed of a semiconductor material portion having a thickness H (nm), a source region formed adjacent to the channel, and a gate-effect region, a field effect transistor disposed in a gate region above the channel, wherein a gate length (L g ) of the gate region is 4 nm or more and 10 nm or less, and a number of doping atoms in a central region of the channel is 1 the following.

又,本發明之第2態樣的場效電晶體之特徵為:其係具備有由厚度H(nm)之半導體材料部所形成的通道、鄰接該通道所形成的源極區域及汲極區域、設置在該通道上方的閘極區域之場效電晶體,其中具備有遮罩層,其係設置在該半導體材料部之主表面上,包含屬於供體或受體之摻雜原子之遮罩層,為設置於該閘極區域之閘極電極的側壁厚度為W(nm)之遮罩層,該遮罩層係覆蓋住形成有該源極區域及汲極區域之該半導體材料部之主表面部,該閘極區域之閘極長度(Lg)為4nm以上10nm以下,該閘極電極之側壁之該遮罩層厚度W(nm)係在[3H -2]/7+[10-Lg]/2≦W≦[3H+19]/7的範圍。 Further, a field effect transistor according to a second aspect of the present invention is characterized in that it has a channel formed of a semiconductor material portion having a thickness H (nm), a source region and a drain region formed adjacent to the channel. a field effect transistor disposed in a gate region above the channel, wherein a mask layer is disposed on the main surface of the semiconductor material portion, and includes a mask of dopant atoms belonging to the donor or the acceptor a layer is a mask layer having a sidewall thickness of W (nm) disposed on a gate electrode of the gate region, the mask layer covering a main portion of the semiconductor material portion in which the source region and the drain region are formed In the surface portion, the gate length (L g ) of the gate region is 4 nm or more and 10 nm or less, and the thickness W (nm) of the mask layer on the sidewall of the gate electrode is in [3H - 2] / 7 + [10- The range of L g ]/2≦W≦[3H+19]/7.

就上述第2態樣的場效電晶體而言,較佳的是該通道之中央區域的摻雜原子數為1以下。 In the field effect transistor of the second aspect described above, it is preferable that the number of doping atoms in the central portion of the channel is 1 or less.

就本發明之場效電晶體而言,較佳的是從該通道端部朝向該源極區域及該汲極區域側之2nm區域的摻雜物濃度為5×1019cm-3以上。 In the field effect transistor of the present invention, it is preferable that the dopant concentration in the 2 nm region from the end portion of the channel toward the source region and the drain region side is 5 × 10 19 cm -3 or more.

該半導體材料部係包括矽、鍺、III-V族化合物半導體之任一材料。 The semiconductor material portion includes any of bismuth, antimony, and III-V compound semiconductors.

例如,該半導體材料部包括矽,該遮罩層為矽氧化膜或矽化物膜。 For example, the semiconductor material portion includes tantalum, and the mask layer is a tantalum oxide film or a vaporized film.

此時,該摻雜物為例如磷、銻、砷、硼、鋁、銦、鎵之任一者。 At this time, the dopant is any one of, for example, phosphorus, antimony, arsenic, boron, aluminum, indium, or gallium.

又,例如,該半導體材料部包括鍺,該遮罩層為鍺氧化膜或鍺化物膜。 Further, for example, the semiconductor material portion includes tantalum, and the mask layer is a tantalum oxide film or a vaporized film.

此時,該摻雜物亦為磷、銻、砷、硼、鋁、銦、鎵之任一者。 At this time, the dopant is also any one of phosphorus, antimony, arsenic, boron, aluminum, indium, and gallium.

再者,例如,該半導體材料部包括III-V族化合物半導體,該遮罩層為矽氧化膜。 Further, for example, the semiconductor material portion includes a III-V compound semiconductor, and the mask layer is a tantalum oxide film.

此時,該摻雜物為鋅、矽、鈹之任一者。 At this time, the dopant is any one of zinc, bismuth, and antimony.

就某態樣而言,該半導體材料部為矽-奈米線、鍺-奈米線、III-V族化合物半導體奈米線之任一者。 In some aspects, the semiconductor material portion is any one of a 矽-nano line, a 锗-nano line, and a III-V compound semiconductor nanowire.

本發明之場效電晶體之製法的特徵為:其係具備由厚度H(nm)之半導體材料部所形成之通道的場效電晶體之製造方法,其具備:以閘極長度(Lg)成為4nm以上10nm以下之方式,在該通道上方形成閘極電極的步 驟;形成遮罩層的步驟,該遮罩層係覆蓋住該閘極電極、及鄰接於該通道之形成有源極區域與汲極區域之該半導體材料部之主表面部的遮罩層,為該閘極電極的側壁厚度為W(nm)之遮罩層;對該遮罩層注入屬於供體或受體之摻雜原子的步驟;使注入至該遮罩層之該摻雜原子擴散到該源極區域與汲極區域的步驟;將該閘極電極之側壁之該遮罩層厚度W(nm)設定於[3H-2]/7+[10-Lg]/2≦W≦[3H+19]/7的範圍。 The method for producing a field effect transistor of the present invention is characterized in that it is a method for producing a field effect transistor having a channel formed of a semiconductor material portion having a thickness H (nm), which is provided with a gate length (Lg) a step of forming a gate electrode over the channel in a manner of 4 nm or more and 10 nm or less; a step of forming a mask layer covering the gate electrode and forming a source region and a region adjacent to the channel a mask layer on a main surface portion of the semiconductor material portion of the polar region is a mask layer having a sidewall thickness of the gate electrode of W (nm); and implanting a dopant atom belonging to the donor or the acceptor to the mask layer a step of diffusing the dopant atoms implanted into the mask layer to the source region and the drain region; setting the thickness W (nm) of the mask layer on the sidewall of the gate electrode to [3H- 2]/7+[10-L g ]/2≦W≦[3H+19]/7 range.

根據本發明的話,可提供一種場效電晶體,其係在半導體奈米線般之半導體材料部的主表面上具備有包含摻雜原子且閘極電極側壁之厚度為W的遮罩層,在通道之中央區域的摻雜原子數為1以下。其結果係可抑制閾值電壓偏差,同時能充分取得導通電流。 According to the present invention, there is provided a field effect transistor which is provided with a mask layer containing a dopant atom and a gate electrode having a thickness W of W on a main surface of a semiconductor nanowire-like semiconductor material portion. The number of doping atoms in the central region of the channel is 1 or less. As a result, the threshold voltage deviation can be suppressed, and the on-current can be sufficiently obtained.

10‧‧‧矽基板 10‧‧‧矽 substrate

20‧‧‧絕緣體膜 20‧‧‧Insulator film

30‧‧‧半導體奈米線 30‧‧‧Semiconductor nanowire

30c‧‧‧通道 30c‧‧‧ channel

30d‧‧‧汲極區域 30d‧‧‧Bungee area

30s‧‧‧源極區域 30s‧‧‧ source area

40‧‧‧閘極電極 40‧‧‧gate electrode

40g‧‧‧閘極區域 40g‧‧‧ gate area

45‧‧‧閘極氧化膜 45‧‧‧Gate oxide film

50‧‧‧遮罩層 50‧‧‧ mask layer

100‧‧‧場效電晶體 100‧‧‧ field effect transistor

H‧‧‧厚度 H‧‧‧thickness

Lg‧‧‧閘極長度 L g ‧‧‧ gate length

td‧‧‧堆積Si氧化膜厚度 t d ‧‧‧Stacked Si oxide film thickness

tg‧‧‧閘極電極高度 t g ‧‧‧gate electrode height

tox‧‧‧閘極氧化膜厚度 t ox ‧‧‧ gate oxide film thickness

W‧‧‧厚度 W‧‧‧thickness

第1圖係用以概念性說明本發明之場效電晶體之構造的剖面圖。 BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a cross-sectional view conceptually illustrating the construction of a field effect transistor of the present invention.

第2圖係就本發明之場效電晶體而言,顯示出用以決定閘極電極側壁之遮罩層厚度W(nm)之適當範圍所進行之模擬結果的圖。 Fig. 2 is a view showing a simulation result of an appropriate range of the thickness W (nm) of the mask layer for determining the sidewall of the gate electrode in the field effect transistor of the present invention.

第1圖係用以概念性說明本發明之場效電晶體之構造的剖面圖。另外,在此圖中,為了簡化說明,圖示了具有1個閘極電極(單一閘極)之構造,但並非限定 於此類態樣,亦可為雙閘極或三閘極構造之電晶體,還可以為通道周圍全視為閘極之構造的電晶體等。 BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a cross-sectional view conceptually illustrating the construction of a field effect transistor of the present invention. In addition, in this figure, in order to simplify the description, a structure having one gate electrode (single gate) is illustrated, but is not limited thereto. In such a form, it may be a transistor of a double gate or a triple gate structure, or a transistor which is constructed as a gate around the channel.

第1圖中所例示之場效電晶體100係具備有由半導體奈米線30所形成之通道30c。鄰接到此通道30c,形成有源極區域30s及汲極區域30d,於通道上方,隔著閘極氧化膜45,設置有閘極電極40,該閘極電極之下方為閘極長度Lg之閘極區域40g。另外,此例中為半導體材料部係半導體奈米線之態樣,然此僅屬例示,構成本發明之半導體電晶體之半導體材料部並非限定於此態樣,只要是可形成通道的半導體材料部即可。 The field effect transistor 100 illustrated in Fig. 1 is provided with a channel 30c formed by a semiconductor nanowire 30. Adjoining this passage 30c, forming a source region 30s and drain region 30d, above the channel, a gate oxide film 45 interposed therebetween, is provided with a gate electrode 40, below the gate electrode to the gate length L g of Gate region 40g. In this example, the semiconductor material portion is a semiconductor nanowire. However, the semiconductor material portion constituting the semiconductor transistor of the present invention is not limited to such an aspect, as long as it is a semiconductor material capable of forming a channel. You can do it.

半導體奈米線30係例如為將SOI基板之半導體層予以加工所獲得之矽-奈米線,或者是在包括n型或p型之傳導型之矽基板10上所形成之矽氧化膜(SiO2)的絕緣體膜20上所設置之矽-奈米線。另外,半導體奈米線並非限定在矽-奈米線,亦可為鍺-奈米線和GaAs等之III-V族化合物半導體奈米線。 The semiconductor nanowire 30 is, for example, a 矽-nano line obtained by processing a semiconductor layer of an SOI substrate, or a tantalum oxide film (SiO formed on a ruthenium substrate 10 including an n-type or p-type conductivity type). 2 ) The tantalum-nano line provided on the insulator film 20. Further, the semiconductor nanowire is not limited to the 矽-nano line, and may be a III-nano line and a III-V compound semiconductor nanowire such as GaAs.

半導體奈米線30係長度與寬度之比(縱橫比)較大之細線狀結晶,其厚度H(nm)係例如為10nm左右。此類半導體奈米線30係可利用絕緣體上之半導體層的加工、或化學氣相堆積法(CVD法)和電漿強化化學氣相堆積法(PECVD法)來形成。在半導體奈米線30為矽-奈米線時,可使用SOI基板來形成半導體奈米線,或者是將矽烷(SiH4)或四氯化矽(SiCl4)氣體當作原料氣體來形成等即可。 The semiconductor nanowire 30 is a thin linear crystal having a large ratio of length to width (aspect ratio), and its thickness H (nm) is, for example, about 10 nm. Such a semiconductor nanowire 30 can be formed by processing a semiconductor layer on an insulator, or by a chemical vapor deposition method (CVD method) or a plasma enhanced chemical vapor deposition method (PECVD method). When the semiconductor nanowire 30 is a 矽-nano line, an SOI substrate can be used to form a semiconductor nanowire, or a silane (SiH 4 ) or a silicon tetrachloride (SiCl 4 ) gas can be formed as a source gas. Just fine.

於半導體奈米線30之主表面上,設置有包含 屬於供體或受體之摻雜原子之遮罩層50。此遮罩層50係例如包括矽氧化膜,以閘極區域40g上方所設置之閘極電極40之側壁厚度成為W(nm)的方式形成,同時覆蓋住形成有源極區域30s及汲極區域30d之半導體奈米線30之主表面部。 On the main surface of the semiconductor nanowire 30, the inclusion is included A mask layer 50 of dopant atoms belonging to a donor or acceptor. The mask layer 50 is, for example, including a tantalum oxide film, and is formed in such a manner that the thickness of the sidewall of the gate electrode 40 provided over the gate region 40g becomes W (nm) while covering the source region 30s and the drain region. The main surface portion of the 30d semiconductor nanowire 30.

遮罩層50係例如在形成矽氧化膜之後,於半導體奈米線30中,離子注入有屬於供體或受體之摻雜原子者。 The mask layer 50 is, for example, after forming a tantalum oxide film, in the semiconductor nanowire 30, ion-implanted with a dopant atom belonging to a donor or a acceptor.

在半導體奈米線30為矽-奈米線的情況下,遮罩層50係除了矽氧化膜之外,亦可為包括矽化物膜之層,作為遮罩層50所包含之摻雜原子,可例示有磷、銻、砷、硼、鋁、銦、鎵。 In the case where the semiconductor nanowire 30 is a 矽-nano line, the mask layer 50 may be a layer including a bismuth film as a doping atom included in the mask layer 50 in addition to the ruthenium oxide film. Phosphorus, antimony, arsenic, boron, aluminum, indium, and gallium are exemplified.

半導體材料部係不限於矽,在第1圖所例示之態樣中,半導體奈米線30亦可為鍺-奈米線。此時,遮罩層50亦可為包括鍺氧化膜和鍺化物膜之層,作為遮罩層50所包含之摻雜原子,可例示有磷、銻、砷、硼、鋁、銦、鎵。 The semiconductor material portion is not limited to ruthenium. In the aspect illustrated in Fig. 1, the semiconductor nanowire 30 may be a 锗-nano line. At this time, the mask layer 50 may be a layer including a tantalum oxide film and a vaporized film, and examples of the dopant atoms contained in the mask layer 50 include phosphorus, germanium, arsenic, boron, aluminum, indium, and gallium.

再者,半導體材料部並不限於矽或鍺,半導體奈米線30亦可為III-V族化合物半導體奈米線。此時,遮罩層50係例如可作成為包括矽氧化膜之層,而作為遮罩層50所包含之摻雜原子,可例示有鋅、矽、鈹。 Further, the semiconductor material portion is not limited to tantalum or niobium, and the semiconductor nanowire 30 may be a III-V compound semiconductor nanowire. At this time, the mask layer 50 can be, for example, a layer including a tantalum oxide film, and examples of the dopant atoms contained in the mask layer 50 include zinc, tantalum, and niobium.

遮罩層50係在製作本發明之場效電晶體時,具有朝向源極區域30s及汲極區域30d之摻雜物之擴散源的作用。 The mask layer 50 functions as a diffusion source for the dopants of the source region 30s and the drain region 30d when the field effect transistor of the present invention is fabricated.

習知係採用如下手法:於例如針對矽-奈米線 之源極區域及汲極區域進行摻雜時,將閘極電極當作為遮罩,將摻雜物直接離子注入至矽-奈米線,其後,藉由進行熱處理,使注入離子電性活化,而作成為供體或受體。然而,就此類手法而言,會有在電晶體本體上因為離子注入所造成之結晶缺陷,且於熱處理後亦會殘留缺陷而使電晶體特性降低的問題。 The conventional method uses the following method: for example, for the 矽-nano line When the source region and the drain region are doped, the gate electrode is used as a mask, and the dopant is directly ion-implanted into the 矽-nano line, and then the implanted ion is electrically activated by heat treatment. And become a donor or acceptor. However, in such a method, there is a problem that crystal defects are caused by ion implantation on the bulk of the transistor, and defects are left after the heat treatment to lower the crystal characteristics.

為了避開此問題而採用所謂的固相擴散法時,摻雜物仍會擴散到電晶體之通道區域,會有電晶體之閾值電壓偏移的問題。另一方面,為了抑制閾值電壓而降低摻雜物濃度時,則會變得無法取得充分的導通電流。 In order to avoid this problem, when the so-called solid phase diffusion method is employed, the dopant still diffuses into the channel region of the transistor, and there is a problem that the threshold voltage of the transistor is shifted. On the other hand, when the dopant concentration is lowered to suppress the threshold voltage, a sufficient on-current cannot be obtained.

依此,就本發明而言,在離子注入前的階段,將遮罩層50形成在包含閘極電極之區域,由此遮罩層50上方進行離子注入。因為離子注入時之損害可由此遮罩層50來吸收,故而可避免對於半導體奈米線30之損害,不會引起結晶缺陷,故不需要用以恢復損害的熱處理。又,遮罩層50係可當作摻雜物之擴散源來作用,而關於可進行何種程度的摻雜,則是可利用離子注入量(摻雜量)來輕易控制。 Accordingly, in the present invention, the mask layer 50 is formed in a region including the gate electrode before the ion implantation, whereby ion implantation is performed over the mask layer 50. Since the damage at the time of ion implantation can be absorbed by the mask layer 50, damage to the semiconductor nanowire 30 can be avoided, and crystal defects are not caused, so that heat treatment for recovering damage is not required. Further, the mask layer 50 functions as a diffusion source of the dopant, and the degree of doping can be easily controlled by the amount of ion implantation (doping amount).

閘極電極40之側壁部的遮罩層50中,也可離子注入摻雜物,而注入離子會留在上方部。亦即,不會注入至接觸到半導體奈米線30之主表面的部分。因此,於閘極電極40之側壁上形成厚度W(nm)的遮罩層部分係不會作用為摻雜物之擴散源。其結果係藉由適當設計此厚度W(nm),則可避免摻雜物朝向通道區域30c的侵入,能減少閾值電壓之偏差,同時可取得充分的導通電流。 In the mask layer 50 of the side wall portion of the gate electrode 40, the dopant may be ion-implanted, and the implanted ions may remain in the upper portion. That is, it is not injected into the portion that contacts the main surface of the semiconductor nanowire 30. Therefore, the portion of the mask layer having a thickness W (nm) formed on the sidewall of the gate electrode 40 does not act as a diffusion source of the dopant. As a result, by appropriately designing the thickness W (nm), the intrusion of the dopant toward the channel region 30c can be avoided, the variation in the threshold voltage can be reduced, and a sufficient on-current can be obtained.

第2圖係顯示出在上述構造之場效電晶體中,用以決定閘極電極40側壁之遮罩層50的厚度W(nm)之適當範圍所進行之模擬結果的圖。橫軸係半導體奈米線之厚度H(nm),縱軸係閘極電極40之側壁之遮罩層50的厚度W(nm)。 Fig. 2 is a view showing a simulation result of an appropriate range for determining the thickness W (nm) of the mask layer 50 on the side wall of the gate electrode 40 in the field effect transistor of the above configuration. The horizontal axis is the thickness H (nm) of the semiconductor nanowire, and the vertical axis is the thickness W (nm) of the mask layer 50 on the sidewall of the gate electrode 40.

此模擬時之條件係如表1所示,於此,將矽氧化膜堆積在包含奈米線MOS場效電晶體(10nm方形以下,長度30nm)之閘極電極的整個面上,自其上離子注入砷之後,透過進行1000℃之熱處理,可使摻雜物擴散。 The conditions in this simulation are shown in Table 1. Here, the tantalum oxide film is deposited on the entire surface of the gate electrode including the nanowire MOS field effect transistor (10 nm square or less, length 30 nm). After ion implantation of arsenic, the dopant can be diffused by heat treatment at 1000 °C.

此處,將離子注入時之加速電壓設為0.5keV,係為了將砷注入至tg為3nm之堆積Si氧化膜中。又,離子注入後,使摻雜物擴散之際的時間係設定為因應半導體奈米線厚度H(nm)之最佳值,為用於將SD(源極/汲極)部摻雜成大致均勻的最短時間,具體來說,因應H=2nm、3nm、5nm、7.5nm、10nm,而為0.25秒、0.5秒、1秒、2.5秒、5秒。 Here, the acceleration voltage at the time of ion implantation was set to 0.5 keV in order to inject arsenic into the deposited Si oxide film having a tg of 3 nm. Further, after ion implantation, the time for diffusing the dopant is set to an optimum value in accordance with the thickness H (nm) of the semiconductor nanowire, and is used for doping the SD (source/drain) portion. The shortest time of uniformity is specifically 0.25 seconds, 0.5 seconds, 1 second, 2.5 seconds, and 5 seconds in response to H = 2 nm, 3 nm, 5 nm, 7.5 nm, and 10 nm.

首先,就厚度W(nm)之上限來說,在自通道端部往源極區域及汲極區域側的2nm中,當依摻雜物(此處是砷)濃度為5×1019cm-3以上之條件來進行評估時,厚度W(nm)之上限值Wu(nm)係成為[3H+19]/7。當為此厚度 以上時,無法取得充分的導通電流。 First, as for the upper limit of the thickness W (nm), in the 2 nm from the end of the channel to the source region and the drain region side, when the concentration of the dopant (here, arsenic) is 5 × 10 19 cm - when the above three conditions to evaluate, on a thickness W (nm) value W u (nm) lines become [3H + 19] / 7. When the thickness is equal to or higher than this, a sufficient on current cannot be obtained.

另外,在自通道端部開始的2nm中,設定摻雜物濃度成為5×1019cm-3以上之條件,係因為在低於此濃度之摻雜物濃度時,會無法取得充分的導通電流所致。 Further, in the case of 2 nm from the end of the channel, the dopant concentration is set to be 5 × 10 19 cm -3 or more because a sufficient on-current cannot be obtained at a dopant concentration lower than the concentration. Caused.

另一方面,就厚度W(nm)之下限來說,在依摻雜物(此處是砷)朝向通道中央之侵入為1以下之條件進行評估時,厚度W(nm)之下限值W1(nm)為[3H-2]/7+[10-Lg]/2。當為此厚度以下時,閾值之偏差會變大。 On the other hand, in the case where the lower limit of the thickness W (nm) is evaluated under the condition that the dopant (here, arsenic) enters the center of the channel to be 1 or less, the thickness W (nm) is lower than the limit W. 1 (nm) is [3H-2]/7+[10-L g ]/2. When the thickness is below this thickness, the deviation of the threshold becomes large.

因此,在本發明中,係將閘極電極40之側壁之遮罩層50厚度W(nm)設定為[3H-2]/7+[10-Lg]/2≦W≦[3H+19]/7之範圍。另外,如由此關係式可知,上限值Wu(nm)不會依存於閘極長度Lg,而下限值W1(nm)會依存於閘極長度LgTherefore, in the present invention, the thickness W (nm) of the mask layer 50 of the sidewall of the gate electrode 40 is set to [3H-2]/7+[10-L g ]/2≦W≦[3H+19 ] / 7 range. Further, as can be seen from this relation, the upper limit value W u (nm) does not depend on the gate length L g , and the lower limit value W 1 (nm) depends on the gate length L g .

就本發明之場效電晶體而言,為了將通道中央區域之摻雜原子數設為1以下,換言之,為了將通道中央區域之摻雜原子數不為2以上,較佳的是閘極區域之閘極長度Lg為4nm以上10nm以下。另外,此處所謂的通道之「中央區域」係意指將通道之幾何學中央位置視為中心之±1nm的區域。此係如上所述,例如,於矽結晶中存在當作為摻雜物之砷原子時,電子自該摻雜物之「流出長度」為2nm(±1nm)左右所致。 In the field effect transistor of the present invention, in order to set the number of doping atoms in the central region of the channel to 1 or less, in other words, in order to make the number of doping atoms in the central region of the channel not more than 2, preferably the gate region The gate length L g is 4 nm or more and 10 nm or less. In addition, the "central region" of the channel herein means an area in which the geometric center position of the channel is regarded as the center of ±1 nm. As described above, for example, when an arsenic atom as a dopant exists in the ruthenium crystal, the "outflow length" of electrons from the dopant is about 2 nm (±1 nm).

如上所述,本發明之場效電晶體係具備有:由厚度H(nm)之半導體奈米線所形成之通道、鄰接於該通道所形成之源極區域及汲極區域、設置在該通道上方之閘極區域,亦具備有遮罩層,其係設置在該半導體奈米 線之主表面上,包含屬於供體或受體之摻雜原子之遮罩層,為設置於該閘極區域之閘極電極的側壁厚度為W(nm)之遮罩層,該遮罩層係覆蓋住形成有該源極區域及汲極區域之該半導體奈米線之主表面部,該閘極區域之閘極長度(Lg)為4nm以上10nm以下,該通道之中央區域的摻雜原子數為1以下。 As described above, the field effect transistor system of the present invention comprises: a channel formed by a semiconductor nanowire having a thickness H (nm), a source region and a drain region formed adjacent to the channel, and disposed in the channel The upper gate region also has a mask layer disposed on the main surface of the semiconductor nanowire, and a mask layer containing doping atoms belonging to the donor or the acceptor is disposed in the gate region a sidewall of the gate electrode having a thickness of W (nm), the mask layer covering a main surface portion of the semiconductor nanowire formed with the source region and the drain region, the gate region The gate length (L g ) is 4 nm or more and 10 nm or less, and the number of doping atoms in the central region of the channel is 1 or less.

上述場效電晶體所具備之遮罩層50係例如包括矽氧化膜,以設置於閘極區域40g上方之閘極電極40之側壁之厚度成為W(nm)的方式形成,同時覆蓋住形成有源極區域30s及汲極區域30d之半導體奈米線30之主表面部,在製作場效電晶體時,可具有當作為朝向源極區域30s及汲極區域30d之摻雜物的擴散源之作用。 The mask layer 50 included in the field effect transistor includes, for example, a tantalum oxide film, and is formed such that the thickness of the sidewall of the gate electrode 40 provided over the gate region 40g becomes W (nm) while covering the formed The main surface portion of the semiconductor nanowire 30 of the source region 30s and the drain region 30d may have a diffusion source as a dopant toward the source region 30s and the drain region 30d when the field effect transistor is fabricated. effect.

就閘極電極40之側壁部的遮罩層50來說,注入離子會留在上方部,而不會注入到接觸半導體奈米線30之主表面的部分。因此,在閘極電極40之側壁上以厚度W(nm)所形成之遮罩層部分係不會當作為摻雜物之擴散源而有所作用。其結果係藉由適當設計此厚度W(nm),則可以避免摻雜物朝向通道區域30c之侵入,可減少閾值電壓之偏差,同時能取得充分的導通電流。 With respect to the mask layer 50 of the side wall portion of the gate electrode 40, the implanted ions remain in the upper portion and are not injected into the portion contacting the main surface of the semiconductor nanowire 30. Therefore, the portion of the mask layer formed by the thickness W (nm) on the sidewall of the gate electrode 40 does not function as a diffusion source of the dopant. As a result, by appropriately designing the thickness W (nm), the intrusion of the dopant toward the channel region 30c can be avoided, the variation in the threshold voltage can be reduced, and a sufficient on-current can be obtained.

如此根據本發明的話,可提供一種場效電晶體,其係具備有遮罩層,其係在半導體奈米線般之半導體材料部之主表面上包含摻雜原子之遮罩層,為閘極電極之側壁厚度為W之遮罩層,通道之中央區域之摻雜原子數為1以下。其結果係可抑制閾值電壓之偏差,同時亦可充分地取得導通電流。 According to the present invention, there is provided a field effect transistor which is provided with a mask layer which is a mask layer containing a dopant atom on a main surface of a semiconductor nanowire-like semiconductor material portion, which is a gate electrode. The sidewall of the electrode has a thickness of W, and the number of doping atoms in the central region of the channel is 1 or less. As a result, the deviation of the threshold voltage can be suppressed, and the on-current can be sufficiently obtained.

[產業上之可利用性] [Industrial availability]

本發明係提供一種具有可抑制閾值電壓偏差,同時能充分取得導通電流之源極-汲極構造,具備由半導體奈米線般之半導體材料部所形成之通道的場效電晶體。 The present invention provides a field effect transistor having a source-drain structure capable of suppressing a threshold voltage deviation and sufficiently obtaining an on-current, and having a channel formed by a semiconductor material portion such as a semiconductor nanowire.

10‧‧‧矽基板 10‧‧‧矽 substrate

20‧‧‧絕緣體膜 20‧‧‧Insulator film

30‧‧‧半導體奈米線 30‧‧‧Semiconductor nanowire

30c‧‧‧通道 30c‧‧‧ channel

30d‧‧‧汲極區域 30d‧‧‧Bungee area

30s‧‧‧源極區域 30s‧‧‧ source area

40‧‧‧閘極電極 40‧‧‧gate electrode

40g‧‧‧閘極區域 40g‧‧‧ gate area

45‧‧‧閘極氧化膜 45‧‧‧Gate oxide film

50‧‧‧遮罩層 50‧‧‧ mask layer

100‧‧‧場效電晶體 100‧‧‧ field effect transistor

H‧‧‧厚度 H‧‧‧thickness

Lg‧‧‧閘極長度 L g ‧‧‧ gate length

td‧‧‧堆積Si氧化膜厚度 t d ‧‧‧Stacked Si oxide film thickness

tg‧‧‧閘極電極高度 t g ‧‧‧gate electrode height

tox‧‧‧閘極氧化膜厚度 t ox ‧‧‧ gate oxide film thickness

W‧‧‧厚度 W‧‧‧thickness

Claims (13)

一種場效電晶體,其係具備有由厚度H(nm)之半導體材料部所形成的通道、鄰接該通道所形成的源極區域及汲極區域、與設置在該通道上方的閘極區域之場效電晶體,其中該閘極區域之閘極長度(Lg)為4nm以上10nm以下,該通道之中央區域的摻雜原子數為1以下。 A field effect transistor comprising a channel formed by a semiconductor material portion having a thickness H (nm), a source region and a drain region formed adjacent to the channel, and a gate region disposed above the channel In the field effect transistor, the gate length (L g ) of the gate region is 4 nm or more and 10 nm or less, and the number of doping atoms in the central region of the channel is 1 or less. 一種場效電晶體,其係具備有由厚度H(nm)之半導體材料部所形成的通道、鄰接該通道所形成的源極區域及汲極區域、與設置在該通道上方的閘極區域之場效電晶體,其中具備有遮罩層,其係設置在該半導體材料部之主表面上,包含屬於供體或受體之摻雜原子之遮罩層,為設置於該閘極區域之閘極電極的側壁厚度為W(nm)之遮罩層,該遮罩層係覆蓋住形成有該源極區域及汲極區域之該半導體材料部之主表面部,該閘極區域之閘極長度(Lg)為4nm以上10nm以下,該閘極電極之側壁之該遮罩層厚度W(nm)係在[3H-2]/7+[10-Lg]/2≦W≦[3H+19]/7的範圍。 A field effect transistor comprising a channel formed by a semiconductor material portion having a thickness H (nm), a source region and a drain region formed adjacent to the channel, and a gate region disposed above the channel a field effect transistor having a mask layer disposed on a main surface of the semiconductor material portion, comprising a mask layer of dopant atoms belonging to a donor or a acceptor, and a gate layer disposed in the gate region a sidewall layer having a sidewall thickness of W (nm), the mask layer covering a main surface portion of the semiconductor material portion in which the source region and the drain region are formed, and a gate length of the gate region (L g ) is 4 nm or more and 10 nm or less, and the thickness W (nm) of the mask layer of the sidewall of the gate electrode is [3H-2]/7+[10-L g ]/2≦W≦[3H+ 19] / 7 range. 如請求項2之場效電晶體,其中該通道之中央區域的摻雜原子數為1以下。 The field effect transistor of claim 2, wherein the number of doping atoms in the central region of the channel is 1 or less. 如請求項1至3中任一項之場效電晶體,其中從該通道端部朝向該源極區域及汲極區域側之2nm區域的摻雜物濃度為5×1019cm-3以上。 The field effect transistor according to any one of claims 1 to 3, wherein a dopant concentration of the 2 nm region from the end of the channel toward the source region and the drain region side is 5 × 10 19 cm -3 or more. 如請求項1至4中任一項之場效電晶體,其中該半導體材料部係包括矽、鍺、III-V族化合物半導體之任一材料。 The field effect transistor of any one of claims 1 to 4, wherein the semiconductor material portion comprises any one of a bismuth, antimony, and III-V compound semiconductor. 如請求項5之場效電晶體,其中該半導體材料部包括矽,該遮罩層為矽氧化膜或矽化物膜。 The field effect transistor of claim 5, wherein the semiconductor material portion comprises germanium, and the mask layer is a tantalum oxide film or a germanide film. 如請求項6之場效電晶體,其中該摻雜物為磷、銻、砷、硼、鋁、銦、鎵之任一者。 The field effect transistor of claim 6, wherein the dopant is any one of phosphorus, germanium, arsenic, boron, aluminum, indium, and gallium. 如請求項5之場效電晶體,其中該半導體材料部包括鍺,該遮罩層為鍺氧化膜或鍺化物膜。 The field effect transistor of claim 5, wherein the semiconductor material portion comprises germanium, and the mask layer is a tantalum oxide film or a germanide film. 如請求項8之場效電晶體,其中該摻雜物為磷、銻、砷、硼、鋁、銦、鎵之任一者。 The field effect transistor of claim 8, wherein the dopant is any one of phosphorus, germanium, arsenic, boron, aluminum, indium, and gallium. 如請求項5之場效電晶體,其中該半導體材料部包括III-V族化合物半導體,該遮罩層為矽氧化膜。 The field effect transistor of claim 5, wherein the semiconductor material portion comprises a III-V compound semiconductor, and the mask layer is a tantalum oxide film. 如請求項10之場效電晶體,其中該摻雜物為鋅、矽、鈹之任一者。 The field effect transistor of claim 10, wherein the dopant is any one of zinc, bismuth, and antimony. 如請求項1至4中任一項之場效電晶體,其中該半導體材料部為矽-奈米線、鍺-奈米線、III-V族化合物半導體奈米線之任一者。 The field effect transistor according to any one of claims 1 to 4, wherein the semiconductor material portion is any one of a 矽-nano line, a 锗-nano line, and a III-V compound semiconductor nanowire. 一種場效電晶體之製造方法,其係具備由厚度H(nm)之半導體材料部所形成之通道的場效電晶體之製造方法,其係具備:以閘極長度(Lg)成為4nm以上10nm以下之方式,在該通道上方形成閘極電極的步驟;形成遮罩層的步驟,該遮罩層係覆蓋住該閘極電極、及鄰接於該通道之形成有源極區域與汲極區域之 該半導體材料部之主表面部,為該閘極電極的側壁厚度為W(nm)之遮罩層;對該遮罩層注入屬於供體或受體之摻雜原子的步驟;使注入至該遮罩層之該摻雜原子擴散到該源極區域與汲極區域的步驟;將該閘極電極之側壁之該遮罩層厚度W(nm)設定於[3H-2]/7+[10-Lg]/2≦W≦[3H+19]/7的範圍。 A method for producing a field effect transistor, comprising a method of manufacturing a field effect transistor having a channel formed by a semiconductor material portion having a thickness H (nm), wherein the gate length (L g ) is 4 nm or more a step of forming a gate electrode over the channel in a manner of 10 nm or less; a step of forming a mask layer covering the gate electrode and forming a source region and a drain region adjacent to the channel a main surface portion of the semiconductor material portion is a mask layer having a sidewall thickness of the gate electrode of W (nm); a step of implanting dopant atoms belonging to the donor or the acceptor into the mask layer; a step of diffusing the dopant atoms of the mask layer to the source region and the drain region; setting the thickness W (nm) of the mask layer on the sidewall of the gate electrode to [3H-2]/7+[ The range of 10-L g ]/2≦W≦[3H+19]/7.
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