• 沒有找到結果。

第五章 結論與未來研究方向

5.2 未來研究方向

在第一章時曾提到,鋁材在歷經400℃以上的製程溫度時,與矽表 面會有相互擴散的情況發生,故在鋁與矽接觸的地方會形成所謂的突 穿現象;要解決此一現象,可以在鋁導線中加入適量的矽,使鋁對矽 的固態溶解度飽和,就可以減少突穿現象發生的機率。在本論文中,

利用鋁的摻雜加強銅膜的抗氧化性及擴散阻擋能力,對銅金屬導線製 程具有正面的幫助。而加入的鋁金屬與矽底材間的擴散作用,也是不 能忽略的,但因本文最主要是找出對銅原子具有最佳擴散阻擋能力的 薄膜,因此鋁與矽之間的相互關係也有待進一步之研究。

第二,擴散阻障層材料的選擇必須符合許多要求;其中,銅膜與 介電層或矽底材之附著性也是個相當重要的參數。金屬導線必然的多 層化發展,在鍍上第一層銅膜後,將還會有後續的化學機械研磨,介 電層沉積、金屬沉積和熱處理製程;另外,利用不同方式所沉積出來 的介電層薄膜或金屬薄膜也會有不同的應力表現。故在不斷的昇溫及 降溫的熱循環中,由溫度所產生疲勞會使得原本熱膨脹係數或應力就 不盡相同的各層材料增加了剥離的機會,對於薄膜的結構及電性的可 靠度會有相當大的影響。本文中原欲藉由鋁與銅的反應生成鋁銅基合 金,以鍵結力較強的金屬鍵取代離子鍵,直接提升擴散阻障層與金屬 薄膜的附著性;但至目前為止,並無有效方法可直接證實銅膜與 Ti-Al-N

的附著性增加與否。因此,擴散阻障層與介電層或矽底材之附著性的 探討和驗證也須再加以證實。

20 25 30 35 40 45 50

Intensity (Arb. Unit)

2θ (degree)

(111) (200) (111) (200) (111) (200)

(111)

圖 4.1 不同氮流量下所沉積的 Ti-Al-N 薄膜經 X 光繞射分析結果。

N2=0 sccm N2=1 sccm N2=2 sccm N2=3 sccm

TiAl

SiO2

圖 4.2 氮流量為零所沉積的 Ti-Al 薄膜經穿透式電子顯微鏡觀察 分析的結果。

20 nm

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 15

20 25 30 35 40 45 50 55 60 65

Resistivity (μΩ-cm)

Nitrogen flow rate (sccm)

Ti-Al-N SiO2

圖 4.3 不同氮流量下所沈積的 Ti-Al-N 薄膜隨電阻率變化的情形。

0 100 200 300 400 500 600 700 800 -5

0 5 10 15 40 60 80 100 120 140

Annealing temperature (

o

C)

Δ R

s

/R

s

N = 0 N = 1 N = 2 N = 3

圖 4.4 Cu/Ti-Al-N/Si 結構經不同溫度退火後片電阻率變化的情形。

圖 4.5 Cu/Ti-Al/Si 經不同退火溫度一小時退火後的 XRD 繞射圖。

圖 4.6 Cu/Ti-Al-N/Si 經不同退火溫度一小時退火後的 XRD 繞射 圖。

20 25 30 35 40 45 50 55

750oC

700oC

650oC

600oC as-dep.

2

θ

(degree)

Intenity (Arb. Unit)

Cu(111)

Cu(200)

Si

Al5Ti3(321)

AlTi3(200)

TiAlN2(102) Cu3Si(320)

0 50 100 150 200 250 300 350 400 100

101 102 103 104 105 106 107

Cu

Al Ti

Si

Secondary ion counts

Sputtering time (sec)

圖 4.7 Cu/Ti-Al /Si 經 550oC 下退火 30 min 後的 SIMS 縱深分佈圖。

0 25 50 75 100 125 150 175 200 225 250 100

101 102 103 104 105 106 107

Ti Cu

Al

N

Si

Secondary ion counts

Sputtering time (sec)

圖 4.8 Cu/Ti-Al-N/Si 經 650oC 下退火 30 min 後的 SIMS 縱深分佈圖。

Cu-Si Cu-Ti-Al

Cu

Si

圖 4.9 Cu/Ti-Al/Si 經 550oC 下退火 30 min 後的 TEM 影像。

100nm

Cu

Ti-Al-N Si

圖 4.10 Cu/Ti-Al-N/Si 經 650oC 下退火 30 min 後的 TEM 影像。

20nm

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