TW464960B - Method of forming a semiconductor thin film - Google Patents

Method of forming a semiconductor thin film Download PDF

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TW464960B
TW464960B TW089114692A TW89114692A TW464960B TW 464960 B TW464960 B TW 464960B TW 089114692 A TW089114692 A TW 089114692A TW 89114692 A TW89114692 A TW 89114692A TW 464960 B TW464960 B TW 464960B
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pulse
thin film
semiconductor thin
energy density
irradiation
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Hiroshi Okumura
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Nippon Electric Co
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    • H01L21/30Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
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Description

464960 五、發明說明(1) 發明背景 發明之領述 本發明係關於一種對非單社 射光進行回火之半導體薄膜之體】膜,射脈衝雷 成在液晶顯示器或密著型影別是關於於形 主办像城測器等絕緣性基板上之客 結晶樣電晶體之活性層之雷射回火製程之構成。 習知拮術 乂 近年,藉由使用複晶矽(以下#p〇ly_Si表示)薄臈 晶體之製造技術,而可形成於廉價之玻璃基驅 電路之液晶顯示裝置。P〇iy-Si薄膜之形成法’由製程溫動 度之低溫化及產能化之觀點而言,使用準分子雷射結晶化 法L其藉由照射準分子雷射光,使非晶矽(以下簡稱為 a - S ΐ )薄膜結晶,而得到p 〇 1 y _ g j薄膜。 ^準分子雷射結晶化法之缺點為:因雷射光為脈衝雷射 光,故薄膜之熱處理時間有限制,使所得之結晶粒之大小 亦被制限。因此,poly —Si薄膜電晶體(TFT)之载子之電場 效果移動度停留於I00cm2/Vs左右,故即使可製成液晶顯琢 不裝置等,亦無法製成DRAM等高頻驅動之高積體電路。 、,poly —Si薄膜之大粒徑化技術之第1技術,如日本特開 平1 0-2 7578 1號公報或第42回應用物理學關係連合演講會开 演講草稿集第2分冊694頁(作者,石原等)所揭示,為以合 成複數脈衝雷射而照射之技術。 又’大粒徑化技術之第2技術,如MRS會刊21期(1 9 96 年)3月號89頁(著者,1爪等)所揭示’為於形成為島狀之非
第5頁
464960 五,發明說明(2) 晶質矽薄膜上’藉由將寬為5 # m之極微細之線狀光束以〇. 7 5 μ m間距掃瞄照射,而形成結晶粒界約成行排列之單方 向生長多結晶矽薄膜之技術。 #明欲解決之誤題 然而’大粒徑化技術之第1技術中,雖然於各雷射照 射領城中進行大粒徑化,但於用於液晶顯示裝置之數百公 釐見方面積之基板中’要均勻地達成大粒徑化極為困難。 又,大粒徑化技術之第2技術中’亦有產能下降之問題, 及為了確保次微米之平台動作精度而使搬送系統複雜化之 問題。 有鑑於上述問題’本發明之目的係在於提供於大面積 基板上高產能,高均一且高移動度之半導體薄膜之製造方 法, 、 解決锞顳之方法 本發明之半導體薄膜之 半導體薄膜以複數脈衝雷射 結晶或單結晶半導體薄膜, 不超過藉由該非單結晶半導 結晶化之能量密度臨界值, 之能量密度,較該非單結晶 而微結晶化之能量密度臨界 衝雷射之前後之脈衝雷射中 後脈衝雷射之能量密度,該 之和超過該能量密度臨界值 製造方法,為藉由對非單結晶 連續於相同處照射,而製造多 其特徵為各脈衝之能量密度, 體薄膜之脈衝雷射之照射而微 該複數脈衝雷射之各脈衝雷射 半導體薄膜藉由脈衝雷射照射 值為低’而於連續之該複數脈 ’别脈衝雷射之能量密度大於 複數脈衝雷射之全部能量密度 ’而該前後脈衝雷射之照射間
五、發明說明(3) 隔’為該前脈衝雷紐 該前後脈衝雷射之寬之脈衝寬之6倍以下,最好 脈衝寬之丨倍以上隔’為該前脈衝雷射之半值宽之 半導該雷射之照射’該多結晶或單結晶 晶粒長度之2 H且# 晶粒長度超過短軸方向之結 之組織,料:罝缺Λ 含於該短軸方向成列並排 行之照射,係為於該非單結晶半導; 轴方向之結晶粒之長度以下之間距,於該 古 丨”: 移動而重覆進行之掃瞄照射。 、 p ^述半導體薄臈之製造方法中,㈣單結晶半導 二ΐνΐΛ壓化學氣相生瞻㈣)法、電漿化學氣相生 ,(PECVD)法、濺鍍法之任—方法而形成,或該多社 早結晶半導體薄膜可形成於玻璃基板上。 、° aa或 較佳實施例之詳細說明 首先,於說明本發明之半導體薄膜之製造方法 之基本的構成前,參考圖3(a),說明成為本發明: 晶化現象。 η京之結 非晶質薄膜及多結晶薄膜等非單結晶構造之薄膜, 稱為非單結晶薄膜’而非單結晶薄膜之微結晶化之產生' 一般係認為藉由薄膜之溶解狀態之變化,使再結晶’ 核產生機構由以基板薄膜界面做為核產生區段之不均一 產生,轉變成均一核產生。此核產生機構之變化,與 ^ 之到達溫度與冷卻速度相關。 … 、
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對非單結晶矽薄膜’以照射如圖3 (a)之具有超過欲結 晶化臨界值Ευ之能量密度之光束形狀之長線狀雷射光時, 於光束形狀上之成為微結晶化臨界值以之正下方之地點, 形成粗大結晶粒。亦即’若見其平面之結晶粒徑分布,則 可於微結晶化區域9之鄰接地點形成粗大結晶粒丨〇。因 此’將光束形狀為非單結晶矽薄膜之微結晶化臨界值以上 之雷射光’照射於非單結晶矽薄膜時,可將所形成之結晶 粒之粒徑及產生位置控制為一次元。特別是將形成於光束 後半部81中之粗大結晶粒1 〇做為種結晶,而以其粒徑以下 掃瞄雷射光時’種.結晶可不間斷地連續生長。因包含以光 束前半部8 0所形成之粗大結晶粒之多結晶組織,藉由其後 之掃瞄照射而微結晶化,故不會妨礙以光束後半部8 1所形 成£種結晶之粒生長。亦即’藉由利用微結晶化現象,可 避免脈衝雷射光掃瞄照射法中之結晶組織不均勻性β 在此,為了得到高產能,最好擴大以光束後半部8丨所 形成之種結晶之結晶粒徑’此可使用於相同處使複數個脈 衝雷射同步,於脈衝寬左右之時間内連續照射之雙重脈衝 法為有效。薄膜藉由於先發脈衝雷射之溶解中,照射次發 脈衝雷射,而延長薄膜之溶解時間,且亦降低凝固速度, 而可擴大結晶粒徑。 本發明之半導體薄膜之製造方法中,如圖1所示,此 雙重脈衝法中,於將η設為1以上之整數時,將第η發之脈 衝能量密度設為Εη ’脈衝寬設為Wn,第(η+1)發之脈衝能 量密度設為Εη+1,第η發之脈衝與第(η + 1)發之脈衝之照
第8頁 464960
Eu>EngEn + l、tnS6Wn、El+E2 + ...+En + En + l>Eu 之條件進 行掃猫照射’而可將具有大粒徑之半導體薄膜大面積均勻 地形成。因此,藉由本發明,可將具有高均一、高移動度 之薄膜電晶體元件形成於大面積基板上。 以下以具體實施型態’說明上述本發明之基本構成。 首先’參考圖2〜5,說明本發明之半導體薄膜之製造 方法之第1實施形態。 射間隔設為tη,薄膜之微結晶化臨界值設為Eu時,藉由將 於玻璃基板1上,藉由電漿化學氣相生長(PECVD)法形 成膜厚為200nm之氧化矽膜2,於其上形成a-Si薄膜8。成 膜法可使用減壓化學氣相生長(LPCVD)法、PECVD法、濺鍍 法等,在此係使用於膜中不含氣體之LPCVD法。膜厚設為 5 Οηίή(圖 5 (a)) 〇 其次,於膜厚50nm之a-Si膜3上,照射具有長邊方向 如為lOOram短邊方向為10〜20 之範圍之波長308nm、脈 衝寬(W1 ) 5 0 n s之X e C1雷射光5 0,此時之微結晶化臨界值 (Eu)為470mJ/cm2。在此,以控制裝置6,使圖2所示之2個 光源4、5同步,透過光學系7,而對設置於反應室8内之玻 璃基板1之a-Si薄膜3,進行雙重脈衝照射。雙重脈衝照射 條件設為:將第1雷射光之能量密度(E1)設為400mJ/cm2、 第2雷射光之能量密度(E2)設為240mJ/cin2、照射間隔(tl) 設為 100ns(tl = 2Fl)。 結果,如圖3 ( a )所示,若進行上述條件之雙重脈衝照 射,則形成具有異向性之橢圓形狀之粗大結晶粒1 〇,其鄰
464960 五、發明說明(6) 接區域成為微結晶化區域9。粗大結 方向11為2.8 βπι,於短軸方士19以9 於長軸 番晰偷昭μ政批尽姐軸方向丨2為1.2 //m。藉由使用本雙 重脈衝照射條件,以粗大結晶粒徑以下之以㈣ 距13進打掃瞒照#,而V得到h圖3(b)所示之連續生長之 ::曰: =67。此時之平台動作精度若考慮粒徑與照射間 此,則寓為ϋ. 7 # m以下。 另一方面,圖3 (c)係為說明本實施形態優點之比較 例。使用雷射結晶化法於以單發照射5〇〇mJ/cm2之雷射光 時,如圖3(c)所示,淤微結晶區域丨9之邊界部形成粒徑 〇, 8私m之約等軸之結晶粒2〇 β為了以此條件連續生長,必 須將掃瞄間距設為〇 · 6 # m以下,而使產能下降。又,因平 台動作精度必須為〇. 2以m以下’故不易穩定地得到於照射 距離全區域連續生長之結晶粒之穩定再現性。 其次’圖4係為改變雷射光之能量密度E1、E2及^ 時’所得之具有異向性之粗大結晶粒之長軸方向之粒徑。 當E1超過Eu時’不論E2及tl為何,其粒徑擴大效果小(圖 4 (a ))。此係由於藉由E丨已使基板界面附近之溫度達到過 份抑制核產生之溫度。為了使當地保持於基板界面之核產 生’以促進粒生長,並將a_Si薄膜之上層溶解,以成為粗 大結晶粒,必須使E1成為Eu以下(圖4 (b )、( c))。又,當 (E1+E2)為Eu以下時,因照射條件,而產生不產生微結晶 化而阻礙連續生長之問題,及因a-Si薄膜上層之溶解不足 而使粒徑擴大效果變小之問題。 其次’參考圖5(b),說明本發明之半導體薄膜之製造
第10頁
464960 五、發明說明(7) 方法之第2實施形態。 於玻璃基板1上’以PECVD法形成lOOnm.之氮化石夕膜22 做為覆膜,接著,以LPCVD法形成膜厚為75iim之a-Si膜 23。對a-Si膜23以波長248nm脈衝寬(W1、W2)為38ns之KrF 雷射光60照射,此時其Eu為500m J/cm2 (圖5(b))。在此, 於以El = 380mJ/cm2、E2 = 260mJ/cni2、E3 = 200mJ/cm2、 tl=80ns、t2 = 50ns(tl=2.1Wl、t2=1.3W2)之條件照射時, 粗大結晶粒之長軸及短軸方向之粒徑,分別為3. 3以m及i. 4#ηι,於長軸方向與短軸方向皆得到較第1實施形態為大 之粒徑。因此,可以較第1實施形態為寬之掃瞄間距進行 掃瞄照射,而使對於平台動作精度之要求較第1實施形態 更為緩和。 **其次,參考圖5(c),說明本發明之半導體薄膜之製造 方法之第3實施形態。 於玻璃基板1,藉由PECVD法形成膜厚為lOOnm之氧化 矽膜42後,同樣地以PECVD法形成膜厚為50nm之a-Si膜 43。在此,因以PECVD法所形成之a-Si膜43較第1、2實施 形態之a-Si膜含有較多量之氫,故進行30分鐘之400 °C之 回火,而進行a-Si膜33之脫氫處理。對a-Si膜43以波長 248nm照射脈衝寬(Wl)38ns之KrF雷射光70,此時其Eu為 460mJ/cm2(圖 5(c))。將KrF 雷射光70 對a-Si 膜43,以 El = 350mJ/cm2、E2 = 200mJ/cm2、tl=60ns(tl = 1.6Wl)之條件 進行照射時,粗大結晶粒之長軸及短軸方向之粒徑,分別 為2.5/zm及l,2"m。於本實施形態中,使用以PECVD法所
第11頁 五、發明說明(8) 形成之a-Si膜時,亦可得到與第1、2實施形態中相同之粗 大結晶粒。因此,可亦約接近第1實施形態之掃瞄間距進 行掃目苗照射’而平台動作精度亦較習知技術大幅改善。 上說明 而言, 衝雷射 佳之關 上所述 ,藉由 向超過 上以大 ,藉由 亦可使 習知更 以 之經驗 於與脈 點,更 發明教 如 a-Si 膜 長轴方 廣範圍 r又 晶粒’ 求,較 之實施形態,僅介紹3個實 用於本發明之複數脈衝雷射之照射間隔t η, 之寬度之關係,滿足t η S 6 W η之關係為重 係則為滿足Wn S tn S4Wn之關係。 ’藉由本發明之半導體薄膜之製造方法,對 照射滿足前述條件之複數脈衝雷射,而得到 短軸方向2倍之粗大結晶粒,而可於基板 掃瞄=距進行掃瞄照射,可得到高產能。 使用前述條件之脈衝雷射照射而得= 將基板對脈衝雷射移動之平台動 声、,、》 大幅緩和,而可大幅減少平台之製;2。
第12頁 464960 圖式簡單說明 圖1 :表示為本發明之半導體薄膜之製造方法之基本構成 部分之互為前後之脈衝雷射之相互關係之脈衝形狀圖。 圖2 :表示使用本發明之半導體薄膜之製造方法之脈衝雷 射之照射裝置及被照射物樣子之模式構成圖。 圖3(a)、圖3(b)、圖3(c):表示藉由本發明之半導體薄膜 之製造方法所得之半導體薄膜之結晶狀態之半導體薄膜之 擴大頂視圖。 圖4(a)、圖4(b)、圖4(c):本發明之半導體薄膜之製造方 法中,將藉由脈衝雷射照射所得之粗大結晶粒之長軸方向 之粒徑與脈衝雷射間隔之關係,以脈衝雷射之能量密度做 為參數表示之圖表。 圖5(a)、圖5(b)、圖5(c):表示使用本發明之半導體薄膜 之製造方法之脈衝雷射之被照射物之樣子之剖面圖。 符號說明 I 玻璃基板 2、 42 氧化矽膜 3、 23、43 a-Si 膜 4 ' 5 光源 6 控制裝置 7 光學系 8 反應室 9、1 9 微結晶化區域 10 粗大結晶粒 II 長軸方向
第13頁 4-6496 Ο 圖式簡單說明 12 短軸方向 13 掃描間距 1 6 結晶粒領城 2 0 結晶粒 22 氮化矽膜 50 XeCl雷射光 60、70 KrF雷射光 80 光束前半部 81 光朿後半部

Claims (1)

  1. 464960
    六、申請專利範圍 _ 1· -種半導體薄臈之製造方法 膜以複數脈衝雷射連續於相同處昭:斜非早結晶H 由該非單結晶半導之能量密度,不超:; 能量密度臨界值。、之脈衝雷射之照射而微結晶化之 2.如申請專利範圍第!項之半導體其 中,^數脈衝雷射之各脈衝雷射之能量密度較該#單 結晶半導體薄膜藉由脈衝雷射照射而微結晶:之能量密度 臨界值為低,而於連續之該複數脈 L 衡雷 ;中=衝雷射之能量密度大於後脈能量密 =界:複數脈衝雷射之全部.能量密度之和超過該能量密度 圍第2項之半導體薄膜之製造方法,其 β 之照射間隔,為該前脈衝雷射之半值 寬之脈衝寬之6倍以下。 4·如申請專利範圍第2項之半導體薄膜之製造方法,其 =,該前後脈衝雷射之照射間㈤,為肖前脈冑雷射之半值 寬之脈衝寬之〗倍以上4倍以下。 · 5 *如申明專利範圍第1至4項中任一項之半導體薄膜之製造 =法,其中,藉由該複數脈衝雷射之照射,令該多結晶或 單結晶半導體薄膜中,長軸方向之結晶粒長度超過短軸方 向之結晶粒長度之2倍,且該結晶教包含於該短韩方向成 列並排之組織。 6.如申請專利範園第5項之半導體薄膜之製造方法,其 第15頁 4 3 6 0 六、申請專利範圍 中,對該非單結晶半導體薄膜以該複數脈衝雷射連續於相 同處所進行之照射,係為於該非單結晶半導體薄膜上,依 結晶粒之長度以下之間距,沿該長軸方向移動,而重覆進 行之掃瞄照射。 7. 如申請專利範圍第5項之半導體薄膜之製造方法,其 中,該非單結晶半導體薄膜可藉由減壓化學氣相生長 (LPCVD)法、電漿化學氣相生長(PECVD)法、濺鍍法之任一 方法而形成。 8. 如申請專利範圍第5項之半導體薄膜之製造方法,其 中,該多結晶或單結晶半導體薄膜可形成於玻璃基板上。
    第16頁
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