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TW201611182A - Method of forming air gap between conductive lines - Google Patents

Method of forming air gap between conductive lines Download PDF

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Publication number
TW201611182A
TW201611182A TW103131773A TW103131773A TW201611182A TW 201611182 A TW201611182 A TW 201611182A TW 103131773 A TW103131773 A TW 103131773A TW 103131773 A TW103131773 A TW 103131773A TW 201611182 A TW201611182 A TW 201611182A
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photoresist
liner
forming
polysilicon
air gap
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TW103131773A
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Chinese (zh)
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TWI562276B (en
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陳品杉
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華邦電子股份有限公司
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Abstract

A method of forming air gap between conductive lines includes forming a SiN liner on surfaces of conductive line structures on a substrate, forming an ultra-thin poly silicon liner covering the SiN liner, and then forming a photoresist in a plurality of trenches between the conductive line structures, wherein a top surface of the photoresist is under that of the conductive line structures. Thereafter, an oxide film is conformally formed to cover the photoresist and a surface of the ultra-thin poly silicon liner, and oxide spacers are formed on sidewalls of the conductive line structures on the photoresist by anisotropic etching the oxide film. Afterwards, the photoresist is removed to expose the ultra-thin poly silicon liner in the trenches, and then the exposed ultra-thin poly silicon liner is removed by using the oxide spacers as mask. The oxide spacers are removed and an oxidation is performed on the remaining ultra-thin poly silicon liner so as to convert it into a silicon oxide layer and close upper portions of the trenches.

Description

在導線間形成空氣間隙的方法 Method of forming an air gap between wires

本發明是有關於一種改善導線間的寄生電容的技術,且特別是有關於一種在導線間形成空氣間隙(air gap)的方法。 The present invention relates to a technique for improving parasitic capacitance between wires, and more particularly to a method of forming an air gap between wires.

半導體元件的發展時至今日已經達數十奈米以下,但是隨著半導體導線結構的線距大幅縮小,升高的寄生電容(parasitic capacitance)卻帶來不良的影響。 The development of semiconductor components has reached tens of nanometers or less, but as the line pitch of semiconductor wire structures has been greatly reduced, the increased parasitic capacitance has adverse effects.

因此,目前的改進方案有在兩導線結構之間的空間沉積較低介電係數(k)值的材料(如氧化物)來取代氮化矽,但是這樣的方式已經不能滿足元件發展到30奈米世代以後的設計。所以近來有在兩導線結構之間的空間,形成空氣間隙來取代氧化物的研究,因為空氣的介電係數(k)值最低。對於空氣間隙的形成,有一部分研究是在導線上沉積非共形(non-conformal)介電質材料,或者是在導線上使用粒徑大於線距的奈米粒子來封閉導線之間的空間。 Therefore, the current improvement has a material that deposits a lower dielectric constant (k) value (such as an oxide) in the space between the two-conductor structure to replace the tantalum nitride, but such a method cannot satisfy the development of the component to 30 nm. The design after the Mi Shidai. Therefore, there has recently been a space between two conductor structures to form an air gap to replace oxides because air has the lowest dielectric constant (k). For the formation of air gaps, part of the study was to deposit a non-conformal dielectric material on the wire, or to use a nanoparticle having a particle size larger than the line spacing on the wire to close the space between the wires.

然而,以上方式有可能形成高度不一致的空氣間隙、或 者奈米粒子填入導線之間的問題。 However, the above method may form a highly inconsistent air gap, or The problem of filling the nanoparticles between the wires.

本發明提供一種在導線間形成空氣間隙的方法,能形成一致的空氣間隙。 The present invention provides a method of forming an air gap between wires to form a uniform air gap.

在本發明的一種在導線間形成空氣間隙的方法中,提供一個在其上形成有數條導線結構的基板,其中每個導線結構至少包括導體層以及位於所述導體層頂部的蓋層。於所述導線結構的表面形成氮化矽襯層,再於所述導線結構上形成多晶矽超薄襯層,覆蓋所述氮化矽襯層。然後,在所述導線結構之間的溝渠內填滿光阻,再移除部分光阻,使光阻的頂面低於導線結構的頂面。之後,在導線結構上共形地形成氧化層,覆蓋光阻與多晶矽超薄襯層的表面。接著,非等向性蝕刻所述氧化層,以於光阻上方的所述導線結構側壁形成氧化物間隙壁,之後移除光阻,以露出溝渠內的所述多晶矽超薄襯層。然後,以氧化物間隙壁為罩幕,去除暴露出的多晶矽超薄襯層,再將氧化物間隙壁移除,使剩餘的多晶矽超薄襯層露出。接著,氧化所述多晶矽超薄襯層,使其轉變為氧化矽層並封閉所述溝渠的上部。 In a method of forming an air gap between wires in accordance with the present invention, a substrate having a plurality of wire structures formed thereon is provided, wherein each wire structure includes at least a conductor layer and a cap layer on top of the conductor layer. A tantalum nitride liner is formed on the surface of the wire structure, and a polysilicon ultrathin liner is formed on the wire structure to cover the tantalum nitride liner. Then, the trench between the wire structures is filled with photoresist, and then part of the photoresist is removed, so that the top surface of the photoresist is lower than the top surface of the wire structure. Thereafter, an oxide layer is conformally formed over the wire structure to cover the surface of the photoresist and the polysilicon ultrathin liner. Next, the oxide layer is anisotropically etched to form an oxide spacer on the sidewall of the wire structure above the photoresist, and then the photoresist is removed to expose the polysilicon ultrathin liner in the trench. Then, using the oxide spacer as a mask, the exposed polycrystalline ultra-thin liner is removed, and the oxide spacer is removed to expose the remaining polycrystalline ultra-thin liner. Next, the polycrystalline silicon ultrathin liner is oxidized to be converted into a ruthenium oxide layer and the upper portion of the trench is closed.

在本發明的一實施例中,上述移除部分光阻的方法包括控制所述光阻的頂面在導體層以上。 In an embodiment of the invention, the method of removing a portion of the photoresist includes controlling a top surface of the photoresist above a conductor layer.

在本發明的一實施例中,上述移除部分光阻的方法包括控制所述光阻的頂面介於蓋層厚度的10%~50%之間。 In an embodiment of the invention, the method of removing a portion of the photoresist includes controlling a top surface of the photoresist to be between 10% and 50% of a thickness of the cap layer.

在本發明的一實施例中,上述多晶矽超薄襯層的厚度在10奈米以下。 In an embodiment of the invention, the polycrystalline germanium ultrathin liner has a thickness of less than 10 nm.

在本發明的一實施例中,上述去除暴露出的多晶矽超薄襯層的方法包括濕式蝕刻。 In an embodiment of the invention, the method of removing the exposed polysilicon ultrathin liner comprises wet etching.

在本發明的一實施例中,上述移除部分光阻的方法包括先對所述光阻進行化學機械研磨,直到露出其頂面,再回蝕刻所述光阻。 In an embodiment of the invention, the method for removing a portion of the photoresist includes chemical mechanical polishing of the photoresist until the top surface is exposed, and etching the photoresist.

在本發明的一實施例中,在上述導線結構上共形地形成氧化層的方法包括原子層沉積法(atomic layer deposition,ALD)。 In an embodiment of the invention, a method of conformally forming an oxide layer on the above-described wire structure includes atomic layer deposition (ALD).

在本發明的一實施例中,上述氧化多晶矽超薄襯層的方法包括自由基氧化法(radical oxidation)或低溫濕式氧化法(low-temperature wet oxidation)。 In an embodiment of the invention, the method for oxidizing the polycrystalline germanium ultrathin liner comprises radical oxidation or low-temperature wet oxidation.

在本發明的一實施例中,在上述氧化多晶矽超薄襯層之前,還可對多晶矽超薄襯層進行磊晶,以增加其厚度。 In an embodiment of the invention, the polycrystalline germanium ultrathin liner may be epitaxially grown to increase its thickness prior to the oxidized polysilicon ultrathin liner.

在本發明的一實施例中,在進行上述磊晶之後,所述多晶矽超薄襯層的所述厚度會增加1.5倍~2倍。 In an embodiment of the invention, the thickness of the polysilicon ultrathin liner is increased by 1.5 times to 2 times after performing the epitaxy.

基於上述,本發明透過控制光阻的頂面,能精確控制空氣間隙的高度,並且藉由導線結構上部的多晶矽超薄襯層的氧化,能完成空氣間隙的封口,達到降低寄生電容的效果。 Based on the above, the present invention can precisely control the height of the air gap by controlling the top surface of the photoresist, and the sealing of the air gap can be completed by the oxidation of the polycrystalline silicon ultra-thin lining on the upper part of the wire structure, thereby achieving the effect of reducing the parasitic capacitance.

為讓本發明的上述特徵和優點能更明顯易懂,下文特舉實施例,並配合所附圖式作詳細說明如下。 The above described features and advantages of the invention will be apparent from the following description.

100‧‧‧基板 100‧‧‧Substrate

102‧‧‧導線結構 102‧‧‧Wire structure

104‧‧‧導體層 104‧‧‧Conductor layer

106‧‧‧蓋層 106‧‧‧ cover

108a、116a‧‧‧頂面 108a, 116a‧‧‧ top

108b‧‧‧側壁 108b‧‧‧ sidewall

110‧‧‧氮化矽襯層 110‧‧‧ nitrided lining

112、112a‧‧‧多晶矽超薄襯層 112, 112a‧‧‧ Polycrystalline silicon ultra-thin lining

114‧‧‧溝渠 114‧‧‧ditch

116‧‧‧光阻 116‧‧‧Light resistance

118‧‧‧範圍 118‧‧‧Scope

120‧‧‧氧化層 120‧‧‧Oxide layer

120a‧‧‧氧化物間隙壁 120a‧‧‧Oxide spacer

122‧‧‧氧化矽層 122‧‧‧Oxide layer

124‧‧‧空氣間隙 124‧‧‧Air gap

200‧‧‧多晶矽磊晶層 200‧‧‧ Polycrystalline germanium epitaxial layer

S1、S2、S3‧‧‧距離 S1, S2, S3‧‧‧ distance

t1、t2、t3、t4‧‧‧厚度 T1, t2, t3, t4‧‧‧ thickness

圖1A至圖1J是依照本發明的一實施例的一種在導線間形成空氣間隙的製造流程剖面示意圖。 1A through 1J are schematic cross-sectional views showing a manufacturing process for forming an air gap between wires in accordance with an embodiment of the present invention.

圖2是本發明的實施例的另一種製程剖面示意圖。 2 is a schematic cross-sectional view showing another process of the embodiment of the present invention.

本文中請參照圖式,以便更加充分地體會本發明的概念,隨附圖式中顯示本發明的實施例。但是,本發明還可採用許多不同形式來實踐,且不應將其解釋為限於底下所述之實施例。實際上,提供實施例僅為使本發明更將詳盡且完整,並將本發明之範疇完全傳達至所屬技術領域中具有通常知識者。 The embodiments of the present invention are shown in the accompanying drawings. However, the invention may be practiced in many different forms and should not be construed as being limited to the embodiments described. Rather, the embodiments are provided so that this disclosure will be thorough and complete, and the scope of the invention will be fully conveyed to those of ordinary skill in the art.

在圖式中,為明確起見可能將各層以及區域的尺寸以及相對尺寸作誇張的描繪。 In the drawings, the dimensions and relative dimensions of the various layers and regions may be exaggerated for clarity.

圖1A至圖1J是依照本發明的一實施例的一種在導線間形成空氣間隙(air gap)的製造流程剖面示意圖。 1A through 1J are schematic cross-sectional views showing a manufacturing process for forming an air gap between wires in accordance with an embodiment of the present invention.

請參照圖1A,在基板100上形成有數條導線結構102,由於本圖是以剖面繪示,所以導線結構102例如長條並延伸在基板100上的線形結構,但本發明並不限於此。每個導線結構102至少包括導體層104以及位於所述導體層104頂部的蓋層106。導體層104可以是單層或多層結構,且與基板100接觸的部分可設置閘氧化層。蓋層106的材料則如氮化矽之類的非導體材料,能 在後續製程期間保護導體層104。此時,導線結構102之間的距離S1為線距(line space);舉例來說,本實施例可適用於半導體製程奈米世代中,所以距離S1約在數十奈米左右,如40奈米以下。 Referring to FIG. 1A, a plurality of wire structures 102 are formed on a substrate 100. Since the figure is shown in cross section, the wire structure 102 is, for example, a linear structure extending over the substrate 100, but the invention is not limited thereto. Each wire structure 102 includes at least a conductor layer 104 and a cap layer 106 on top of the conductor layer 104. The conductor layer 104 may be a single layer or a multilayer structure, and a portion in contact with the substrate 100 may be provided with a gate oxide layer. The material of the cap layer 106 is a non-conductor material such as tantalum nitride. The conductor layer 104 is protected during subsequent processing. At this time, the distance S1 between the wire structures 102 is a line space; for example, the embodiment can be applied to the semiconductor process in the nano generation, so the distance S1 is about several tens of nanometers, such as 40 Below the meter.

然後,請參照圖1B,於基板100上形成氮化矽襯層110,其厚度僅數奈米,故可完整包覆圖1B中的結構之頂面108a與側壁108b。此時,距離S2會比圖1A中的距離S1進一步縮短。 Then, referring to FIG. 1B, a tantalum nitride liner 110 is formed on the substrate 100, and the thickness thereof is only a few nanometers, so that the top surface 108a and the sidewall 108b of the structure in FIG. 1B can be completely covered. At this time, the distance S2 is further shortened than the distance S1 in FIG. 1A.

接著,請參照圖1C,形成多晶矽超薄襯層112,覆蓋所述氮化矽襯層110。在本實施例中,所謂的多晶矽超薄襯層112是指厚度t1在10奈米以下的超薄膜,而厚度t1的大小基本上取決於圖1A的距離S1,較佳是約3nm~5nm之間,且其形成方法例如使用矽烷(silane)為原料、或者使用反應速率較快的乙矽烷(disilane)為原料,以形成緻密且平坦的超薄膜。在多晶矽超薄襯層112形成後,溝渠114的寬度(即距離S3)會進一步縮小。 Next, referring to FIG. 1C, a polysilicon ultrathin liner 112 is formed to cover the tantalum nitride liner 110. In the present embodiment, the so-called polysilicon ultrathin liner 112 refers to an ultrathin film having a thickness t1 of 10 nm or less, and the thickness t1 is basically determined by the distance S1 of FIG. 1A, preferably about 3 nm to 5 nm. In the meantime, the formation method is, for example, using silane as a raw material or using a disilane having a relatively high reaction rate as a raw material to form a dense and flat ultrathin film. After the polysilicon ultrathin liner 112 is formed, the width of the trench 114 (i.e., the distance S3) is further reduced.

然後,請參照圖1D,在導線結構102之間的溝渠114內填滿光阻116,例如用塗佈的方式將光阻116形成於基板100上。 Then, referring to FIG. 1D, the trenches 114 between the wire structures 102 are filled with the photoresist 116, and the photoresist 116 is formed on the substrate 100, for example, by coating.

接著,請參照圖1E,移除部分光阻116,使光阻116的頂面116a低於頂面108a。而且,因為頂面116a的位置將會影響後續形成的空氣間隙的高度,所以可進一步控制光阻116的頂面116a在導體層104以上。舉例來說,所述光阻116的頂面116a可控制在蓋層106厚度t2的10%~50%之間的範圍118內。至於移除部分光阻116的方法例如對圖1D的光阻116進行化學機械研磨,直到露出多晶矽超薄襯層112頂面,再回蝕刻所述光阻116。 Next, referring to FIG. 1E, a portion of the photoresist 116 is removed such that the top surface 116a of the photoresist 116 is lower than the top surface 108a. Moreover, because the location of the top surface 116a will affect the height of the subsequently formed air gap, the top surface 116a of the photoresist 116 can be further controlled above the conductor layer 104. For example, the top surface 116a of the photoresist 116 can be controlled within a range 118 between 10% and 50% of the thickness t2 of the cap layer 106. As for the method of removing a portion of the photoresist 116, for example, the photoresist 116 of FIG. 1D is chemically mechanically polished until the top surface of the polysilicon ultrathin liner 112 is exposed, and the photoresist 116 is etched back.

之後,請參照圖1F,在導線結構102上共形地形成氧化層120,以將光阻116與多晶矽超薄襯層112的表面覆蓋。形成氧化層120的方法例如原子層沉積法(atomic layer deposition,ALD),且沉積製程的溫度例如在60℃~80℃之間。 Thereafter, referring to FIG. 1F, an oxide layer 120 is conformally formed on the wire structure 102 to cover the surface of the photoresist 116 and the polysilicon ultrathin liner 112. A method of forming the oxide layer 120 is, for example, atomic layer deposition (ALD), and the temperature of the deposition process is, for example, between 60 ° C and 80 ° C.

接著,請參照圖1G,非等向性蝕刻圖1F的氧化層120,以於光阻116上方的導線結構102側壁108b形成氧化物間隙壁120a,並露出多晶矽超薄襯層112的頂部與部分光阻116。 Next, referring to FIG. 1G, the oxide layer 120 of FIG. 1F is anisotropically etched to form an oxide spacer 120a on the sidewall 108b of the wire structure 102 above the photoresist 116, and expose the top and the portion of the polysilicon ultra-thin liner 112. Photoresist 116.

然後,請參照圖1H,將所有光阻116移除,使溝渠114內的多晶矽超薄襯層112露出,再以氧化物間隙壁120a為罩幕,例用如濕式蝕刻之類的方式去除暴露出的多晶矽超薄襯層112,直到露出氧化物間隙壁120a底下之溝渠114內的氮化矽襯層110。由於濕式蝕刻是等向性蝕刻,所以被氧化物間隙壁120a遮住的多晶矽超薄襯層112a會稍微內縮。 Then, referring to FIG. 1H, all the photoresists 116 are removed, and the polysilicon ultra-thin liner 112 in the trenches 114 is exposed, and then the oxide spacers 120a are used as a mask, for example, by wet etching or the like. The exposed polysilicon ultrathin liner 112 is exposed until the tantalum nitride liner 110 within the trench 114 under the oxide spacer 120a is exposed. Since the wet etching is an isotropic etching, the polysilicon ultrathin liner 112a covered by the oxide spacer 120a is slightly retracted.

然後,請參照圖1I,將圖1H中的氧化物間隙壁移除,使剩餘的多晶矽超薄襯層112a露出。 Then, referring to FIG. 1I, the oxide spacers in FIG. 1H are removed to expose the remaining polysilicon ultra-thin liner 112a.

接著,請參照圖1J,氧化圖1I的多晶矽超薄襯層112a,使其轉變為氧化矽層122,由於氧化後體積會膨脹約1.6倍,所以氧化矽層122能封閉溝渠的上部,而在導線結構102之間形成空氣間隙124。氧化多晶矽超薄襯層112a的方法例如自由基氧化法(radical oxidation)或低溫濕式氧化法(low-temperature wet oxidation),以便在較低溫度下使多晶矽超薄襯層112a完全轉變為氧化矽層122,但本發明並不限於此。 Next, referring to FIG. 1J, the polysilicon ultra-thin liner 112a of FIG. 1I is oxidized to be transformed into the ruthenium oxide layer 122. Since the volume is expanded by about 1.6 times after oxidation, the ruthenium oxide layer 122 can close the upper portion of the trench. An air gap 124 is formed between the wire structures 102. A method of oxidizing the polycrystalline germanium ultrathin liner 112a such as radical oxidation or low-temperature wet oxidation to completely convert the polycrystalline germanium ultrathin liner 112a to hafnium oxide at a lower temperature Layer 122, but the invention is not limited thereto.

由圖1J可知,導線結構102之間除了氮化矽襯層110以外並無其他結構存在,所以即使半導體線距逐漸變小,仍能確保空氣間隙124的有效距離,而且在本實施例中,透過在移除部分光阻116時控制頂面116a的高度,可在後續的步驟中製作出位置與高度一致的空氣間隙124。 As can be seen from FIG. 1J, there is no other structure between the wire structures 102 except the tantalum nitride liner layer 110, so even if the semiconductor line pitch is gradually reduced, the effective distance of the air gap 124 can be ensured, and in this embodiment, By controlling the height of the top surface 116a when removing a portion of the photoresist 116, an air gap 124 having a position and height can be produced in a subsequent step.

另外,在圖1I中的多晶矽超薄襯層112a假使如圖2所示,其厚度t3可能在氧化後仍無法封閉蓋層106之間的空間,因此可先對多晶矽超薄襯層112a進行磊晶,藉由成長出來的多晶矽磊晶層200來增加整體厚度。之後可進行圖1J的步驟。在進行所述磊晶期間,因為基板100與導體層104等結構都被氮化矽襯層110覆蓋,所以並不會長出磊晶層。而在磊晶之後,多晶矽超薄襯層的厚度t4例如增加1.5倍~2倍,但本發明並不限於此。 In addition, the polycrystalline silicon ultrathin liner 112a in FIG. 1I may have a thickness t3 which may not close the space between the cap layers 106 after oxidation, so that the polycrystalline germanium ultrathin liner 112a may be first exposed. The crystal is increased in thickness by the grown polycrystalline germanium epitaxial layer 200. The steps of Figure 1J can then be performed. During the epitaxial deposition, since the structures of the substrate 100 and the conductor layer 104 are covered by the tantalum nitride liner 110, the epitaxial layer is not grown. After the epitaxy, the thickness t4 of the polycrystalline silicon ultra-thin liner is increased by, for example, 1.5 times to 2 times, but the present invention is not limited thereto.

綜上所述,本發明的方法能藉由光阻控制空氣間隙的高度,且通過氧化位於導線結構上部的多晶矽超薄襯層,來幫助空氣間隙的封口。 In summary, the method of the present invention can control the height of the air gap by the photoresist and help seal the air gap by oxidizing the polysilicon ultrathin liner located on the upper portion of the wire structure.

雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。 Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention, and any one of ordinary skill in the art can make some changes and refinements without departing from the spirit and scope of the present invention. The scope of the invention is defined by the scope of the appended claims.

100‧‧‧基板 100‧‧‧Substrate

102‧‧‧導線結構 102‧‧‧Wire structure

104‧‧‧導體層 104‧‧‧Conductor layer

106‧‧‧蓋層 106‧‧‧ cover

108b‧‧‧側壁 108b‧‧‧ sidewall

112‧‧‧多晶矽超薄襯層 112‧‧‧Polysilicon ultra-thin lining

116‧‧‧光阻 116‧‧‧Light resistance

120a‧‧‧氧化物間隙壁 120a‧‧‧Oxide spacer

Claims (10)

一種在導線間形成空氣間隙的方法,包括:提供基板,在所述基板上形成有多數條導線結構,其中每個所述導線結構至少包括導體層以及位於所述導體層頂部的蓋層;於所述導線結構的表面形成氮化矽襯層;於所述導線結構上形成多晶矽超薄襯層,覆蓋所述氮化矽襯層;在所述導線結構之間的溝渠內填滿光阻;移除部分所述光阻,使所述光阻的頂面低於所述導線結構的頂面;在所述導線結構上共形地形成氧化層,覆蓋所述光阻與所述多晶矽超薄襯層的表面;非等向性蝕刻所述氧化層,以於所述光阻上方的所述導線結構側壁形成氧化物間隙壁;移除所述光阻,以露出所述溝渠內的所述多晶矽超薄襯層;以所述氧化物間隙壁為罩幕,去除暴露出的所述多晶矽超薄襯層;移除所述氧化物間隙壁,以露出所述多晶矽超薄襯層;以及氧化所述多晶矽超薄襯層,使其轉變為氧化矽層並封閉所述溝渠的上部。 A method of forming an air gap between wires, comprising: providing a substrate on which a plurality of wire structures are formed, wherein each of the wire structures includes at least a conductor layer and a cap layer on top of the conductor layer; Forming a tantalum nitride liner on the surface of the wire structure; forming a polysilicon ultra-thin liner on the wire structure to cover the tantalum nitride liner; filling the trench between the wire structures with a photoresist; Removing a portion of the photoresist such that a top surface of the photoresist is lower than a top surface of the wire structure; forming an oxide layer conformally on the wire structure, covering the photoresist and the polysilicon thin a surface of the liner; anisotropically etching the oxide layer to form an oxide spacer on the sidewall of the wire structure above the photoresist; removing the photoresist to expose the inside of the trench a polysilicon ruthenium liner; removing the exposed polysilicon ultrathin liner with the oxide spacer as a mask; removing the oxide spacer to expose the polysilicon ultrathin liner; and oxidizing The polycrystalline silicon ultrathin liner Turn it into a silicon oxide layer and an upper portion of said closed trench. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中移除部分所述光阻的方法包括控制所述光阻的所述頂面 在所述導體層以上。 A method of forming an air gap between wires as described in claim 1, wherein the method of removing a portion of the photoresist comprises controlling the top surface of the photoresist Above the conductor layer. 如申請專利範圍第2項所述的在導線間形成空氣間隙的方法,其中移除部分所述光阻的方法包括控制所述光阻的所述頂面介於所述蓋層的厚度的10%~50%之間。 A method of forming an air gap between wires according to claim 2, wherein the method of removing a portion of the photoresist comprises controlling the top surface of the photoresist to be 10 of a thickness of the cap layer Between %~50%. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中所述多晶矽超薄襯層的厚度在10奈米以下。 A method of forming an air gap between wires according to claim 1, wherein the polysilicon ultrathin liner has a thickness of 10 nm or less. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中去除暴露出的所述多晶矽超薄襯層的方法包括濕式蝕刻。 A method of forming an air gap between wires as described in claim 1, wherein the method of removing the exposed polysilicon ultrathin liner comprises wet etching. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中移除部分所述光阻的方法包括:對所述光阻進行化學機械研磨,直到露出所述多晶矽超薄襯層的頂面;以及回蝕刻所述光阻。 A method of forming an air gap between wires according to claim 1, wherein the method of removing a portion of the photoresist comprises: chemical mechanical polishing the photoresist until the polysilicon ultrathin liner is exposed a top surface; and etch back the photoresist. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中在所述導線結構上共形地形成所述氧化層的方法包括原子層沉積法(atomic layer deposition,ALD)。 A method of forming an air gap between wires as described in claim 1, wherein the method of conformally forming the oxide layer on the wire structure comprises atomic layer deposition (ALD). 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中氧化所述多晶矽超薄襯層的方法包括自由基氧化法或低溫濕式氧化法。 A method of forming an air gap between wires according to claim 1, wherein the method of oxidizing the polysilicon ultrathin liner comprises a radical oxidation method or a low temperature wet oxidation method. 如申請專利範圍第1項所述的在導線間形成空氣間隙的方法,其中在氧化所述多晶矽超薄襯層之前,更包括對所述多晶矽超薄襯層進行磊晶,以增加所述多晶矽超薄襯層的厚度。 The method of forming an air gap between wires according to claim 1, wherein before oxidizing the polysilicon ultrathin liner, the epitaxial layer of the polysilicon ultrathin liner is further included to increase the polysilicon. The thickness of the ultra-thin liner. 如申請專利範圍第9項所述的在導線間形成空氣間隙的方法,其中在進行所述磊晶之後,所述多晶矽超薄襯層的所述厚度增加1.5倍~2倍。 The method of forming an air gap between wires according to claim 9, wherein the thickness of the polysilicon ultrathin liner is increased by 1.5 times to 2 times after the epitaxing.
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