TW200912252A - Method of predicting polishing end time - Google Patents
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- TW200912252A TW200912252A TW97118981A TW97118981A TW200912252A TW 200912252 A TW200912252 A TW 200912252A TW 97118981 A TW97118981 A TW 97118981A TW 97118981 A TW97118981 A TW 97118981A TW 200912252 A TW200912252 A TW 200912252A
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- conductive film
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- 238000005498 polishing Methods 0.000 title claims abstract description 157
- 238000000034 method Methods 0.000 title claims description 60
- 230000002500 effect on skin Effects 0.000 claims abstract description 32
- 238000012544 monitoring process Methods 0.000 claims abstract description 16
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- 239000003990 capacitor Substances 0.000 claims description 12
- 239000000463 material Substances 0.000 claims description 12
- 238000005259 measurement Methods 0.000 claims description 9
- 238000007517 polishing process Methods 0.000 claims description 8
- 239000007788 liquid Substances 0.000 claims description 6
- 239000013078 crystal Substances 0.000 claims description 5
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- 239000010408 film Substances 0.000 description 341
- 230000010355 oscillation Effects 0.000 description 45
- 239000004020 conductor Substances 0.000 description 32
- 238000001514 detection method Methods 0.000 description 31
- 239000010949 copper Substances 0.000 description 20
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- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 230000009471 action Effects 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 2
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- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
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- 241000282326 Felis catus Species 0.000 description 1
- ISWSIDIOOBJBQZ-UHFFFAOYSA-N Phenol Chemical compound OC1=CC=CC=C1 ISWSIDIOOBJBQZ-UHFFFAOYSA-N 0.000 description 1
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- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
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- 229910052742 iron Inorganic materials 0.000 description 1
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Landscapes
- Mechanical Treatment Of Semiconductor (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Finish Polishing, Edge Sharpening, And Grinding By Specific Grinding Devices (AREA)
Abstract
Description
200912252 九、發明說明: 〔發明所屬技術領域〕 〔0001〕 本發明係有關,在進行研磨被形成於半導體晶圓上的 導電性骐時之研磨結束時間點的預測方法者,特別是有關 使用了電感器而從導電性膜的振盪頻率之特徵的變化,檢 出研磨狀態及預測研磨結束時間點之研磨結束時間點的預 測方法者。 〔先前技術〕 〔 0002〕 可知有-製程為,在半導趙晶圓的表面形成例如氧化 膜,對氧《針平版㈣iKmhQgraphy)及關㈣成與 配線圖案對應的溝狀圖案之後,在其上成膜有以充填溝狀 圖案用的Cu等所構成之導電性膜,再利用化學機械研磨來 除去该導電性膜中的溝狀圖案或通孔部份等之埋人部以外 的不要部份㈣成配線圖案。以此配_案之形成而古, 確實地檢出不要的部份之導電,_6被適當除去厚度時之 研磨終點並停止製程是重要的。當過度研料電性膜時會 使配線的電阻增加,研磨過少時則會導致配線絶緣障礙。 〔 0003〕 在與研磨狀態之監視方法有關連的習知技術方面,例 如專利文獻1公開了當場監視薄膜厚度之變化的方法。此 =知技術為’在利用化學機械研磨而從基底本雜(半導趙 晶園)上除去導電性薄膜之方法中,當場監視該導電性薄 膜之厚度變化的方法’係作成將含有由捲成鐵氧罐型的線 200912252 圏所成的電感器與電容器之串聯或並聯的共振電路之感測 器與前述導電性薄膜接近地作配置,將來自高頻激勵信號 源的掃描輸出,透過動作點設定用阻抗手段而朝感測器施 加’藉此’當感測器被激勵時,振盪電流在線圈流動,產生 交替電磁場(alternating electromagnetic field)。此交 替電磁場接著在導電性薄膜中誘導渴電流^當渦電流被誘 導於導電性薄膜時,產生二個效果。第一,導電性薄膜作 為損失電阻作用,其效果為針對於感測電路之電阻負荷, 此乃降低共振信號的振幅,降低共振頻率。第二,當導電 性薄膜的厚度減少時,產生與配置在電感器之線圏中心的 金屬桿被拔出同樣的效果,依此而引起電感的變化以及頻 率平移。透過這樣監視與起因於導電性薄膜厚度變化之感 測器的共振峰值相關連的頻率平移,而連續地檢出該導電 性薄膜之厚度變化》 〔 0004〕 又有關其他的習知技術方面’可知有例如以下那樣 的渦電流感測器(專利文獻2)。此專利文獻2為,在先行 技術方面,係以一般在半導體基板的表面所設之導電性膜 形成渦電流,渦電流感測器依此渦電流間接地進行膜厚之 計測的習知技術中,難以進行正確賴厚檢出困難為問題 點(段S GGG4)’而提供從形成於半導趙基板上之極薄的 膜厚到較厚的導電性膜都能正4地進行膜厚等之檢出的渴 電流感測器為目的(段落0005 ) » 〔 0005〕 於是,在此文獻中,具備有配置在導電性膜或是形成 200912252 有導電性膜的基體附近的感測線圈(渦電流感測器),對該 感測線圈供給一定頻率的交流信號以於前述導電性膜上形 成渦電流用的交流信號源、以及計測含有前述導電性膜的 電抗成份及電阻成份的檢測電路,前述感測線圈係具備與 信號源連接的振盪線圈、配置在振盪線圈之導電性膜側的 檢測線圏、以及配置在振盪線圈的導電性膜側之相反側的 平衡線圈’並以與檢測線圈及平衡線圈互呈反相的方式作 連接。 然後’由前述檢測電路所檢測的電阻成份及電抗成份 輸出合成阻抗,再由阻抗之變化,在寬廣的範圍中把前述 導電性膜之膜厚變化當成大約直線關係來進行檢測。 〔 0006〕 在專利文獻2的情況,例如使渦電流在較厚的膜產生 並測定膜厚’另一方面,研磨該厚膜使之減少而使渦電流 量持續減少時,在其渦電流既減少的分量中,磁場的能量 未在表面的導電性膜被單純地消耗,維持原樣進入到位在 導電性膜之下的元件内部《亦即,對於本來要在導電性膜 被消耗之磁場的能量,隨著導電性膜被除去,而容許元件 内部暴露於過剩的磁場的能量者。 〔 0007 ] 再者,有關其他習知技術方面,可知有例如以下那樣 的渴電流感測器(專利文獻3 )。首先,作為先行技術方面, 於(段落0012),依習知之渦電流感測器的研磨終點之檢 出方法為,在渦電流感測器使用的振盪頻率為7MHz左右, 由於較小,所以在研磨對象的導電性膜夠厚的情況可檢出 200912252 大的渦電流損,但是當導電性膜的研磨進行 而膜厚變得極 薄時,渦電流損的大小係變小,在此情況難以檢出例如丨〇〇〇 a以下程度的膜厚。亦即,習知的渦電流感測器由於振盪 • 頻率較低’所以在被要求是埃等級的膜厚檢出精度之研磨 裝置的研磨終點之檢出上,有所謂其精度不足的問題。 〔 0008〕 在此’揭示了不論是厚的膜厚或是薄的膜厚,都同樣 地使磁場侵入於膜内,依基於其磁場的渦電流大小來單純 地監視膜厚之方法。專利文獻3的技術也與先前所示的習 知技術同樣地’感測器線圈所形成之磁力線貫通被配置在 其感測器線圈全面之基板上的導電性膜並交替地變化,藉 此使渦電流產生於導電性膜中,透過其渦電流在導電性膜 .中流通而產生渦電流損失,以等效電路來看,作成使感測 器線圈之阻抗的電抗成份降低(段落〇008)β 〔 0009〕 又,透過觀察振盪電路之振盪頻率的變化,伴隨著研 磨的進行,導電性膜除變薄時,振盪頻率依此而降低,當 導電性膜因研磨而變得完全沒有時’成為槽電路之本身振 盪頻率,在那以後,振盪頻率略成為一定》因此,透過檢 出此點’能檢出導電性膜之依化學機械研磨的終點(段落 0009 )。 〔0010〕 又’如該文獻中之圖2所示,導電性膜的研磨一進行 時,伴隨的是渦電流損變化,感測器線圏之等價的電阻值 係變化。因此,由於振盪電路之振盪頻率會變化,所以透 200912252 過以除頻電路將此振盈信號除頻,或利用減法器進行減法 計算,而將對應於檢出寬度之頻率大小的信號顯示於監視 器。依此可獲得上述圖2所示那樣的頻率軌跡之推移(段 落 0025)。 、 C 0011) 再者,也知道有如次那樣的渦電流感測器(專利文獻 4)。此文獻的中請專利脑帛!項為—種滿電流感測器, 係具備有配置在形成有導電性膜的基板之近傍的感測器線 圈、對该感測器線圈供給交流信號而在導電性膜形成渦電 流的信號源、以及把形成於導電性膜的渦電流作為由感測 器線圈所見的阻抗予以檢出的檢出電路,該满電流感測器 之特徵為,前述感測器線圏係修正於由高透磁率材料所形 成的收容構件内。 〔0012〕 又,在此文獻之申請專利範圍第7項中係揭示一種渦 電流感測器’其具備有配置在形成有導電性膜或導電性膜 的基板之近傍的感測器線圈、對該感測器線圈供給交流信 號而在前述導電性膜形成渦電流的信號源、以及將形成於 前述導電性膜的渦電流作為由前述感測器線圈所見的阻抗 予以檢出的檢出電路,該渦電流感測器之特徵為,將前述 阻抗的電阻成份與電抗成份顯示直角座標軸上,從與連結 前述阻抗的座標與所指定的中心點之座標的直線所成之角 度來檢出前述導電性膜之膜厚。 [專利文獻1〕專利第2878178號公報(第2頁〜第7 頁’圖1〜圖15)。 200912252 〔專利文獻2〕專利第3587822號公報(第3頁,圖夏 〜圖11)〇 〔專利文獻3〕專利第39〇2〇64號公報 〔專利文獻4〕特開2005-121616號 〔發明内容〕 〔發明所欲解決之課題〕 〔0013〕 在專利文獻1之薄膜厚度的監視方法中,於感測器使 用了由捲繞在讓電磁場具有指向性用的鐵氧罐型怒之線圈 所成的電感器與電容器之串聯或並聯共振電路。接著,在 研磨初期將20Hz〜40. 1MHz的頻率所成的掃描輸出朝感測 器施加,藉由前述線圏所發生之具指向性的交替電磁場,產 生貫通導電性4顧的漏③磁力線且從研磨初期誘導與該 導電性薄膜之膜厚對應之大的渴電流。 〔0014〕 為了誘導與導電性薄膜之膜厚相對應之大的渴電流, 需要大的交替電磁場,亦即形成可貫通導電性薄膜之程度 之大的磁力線是必要的,導電性薄膜之厚度變化的監視係 利用從研磨油到研磨終期、在導電性薄_所引起之渴 電流而進行著。因此,在監視骐厚變化的期間,有必要使 磁力線朝導電性薄膜之厚度方向貫通。在專利文獻丨之圖 面中,從全部的導電性薄膜之部分所記載之貫通導電性薄 膜的磁力線就可清楚。 〔0015〕 10 200912252 在研磨初期之晶圓的表面,通常無垢的Cu膜(導電性 薄膜)是位在最上層。為了在此等無垢的Cu膜全部之上誘 發满電流而有需要非常大的漏洩磁力線。但是,其漏洩磁 力線雖然可誘發渦電流,但是其等係皆以所謂渦電流損失的 形態成為焦耳熱而被消耗《此焦耳熱損,針對最表層之無 垢Cu膜,因體積電阻小故發熱較小,而内部已被配線的部 份,配線剖面積小而體積電阻大,故依貫通的磁力線而誘 發大的渦電流,其結果係局部地產生大的焦耳熱損。這偶 爾會發展成一部份配線熔融、斷線的問題。成為所謂的誘 導加熱之狀態’特別是成為造成在内部悶熱的現象。特別 是’以Cu配線等而言’擔心Cu被加熱後Cu會在Ta等之 阻播膜上擴散的情況、或是依場合而突破阻播膜造成〇11擴 散的情況。 〔0016〕 又’在晶圓之表面部施作有好幾層配線的場合中,不 僅是擔心表層的Cu膜,有時也會有在已處理完了之内部的 配線部份被局部地溫熱而擴散到周圍、或是形成半導趙基 板内的P型、η型的攙雜物再擴散並改變基板内元件的特 性之情況。又,即使是未產生熱的場合,在使過剩的渦電 流流通於微細配線之場合,有時會引發電遷移而造成斷線。 〔0017〕 朝元件侵入的磁場造成元件的損害可作如次的解釋。 亦即,專利文獻1的方法中,在表面的導電性膜(Cu膜) 之部分,依侵入進來的磁場形成渦電流,依其渦電流而產 生斥力磁場。在研磨初期,由於透過覆盖表面的導電性膜 200912252 J防止磁場朝内部元件侵入’故對元件的損害小。在能量 面:透過由覆蓋表面的導電性膜產生的渦電流,作為焦 耳熱知在導電性膜内被消耗。因此,在研磨初期,内部元 件係受表面的導電性膜保護免部分磁場的影響。 〔0018〕 但是,當研磨進行而除去覆蓋表面的導電性膜之膜 時,磁場就這樣在未被減輕之下侵入到元件内。在研磨初 期’,雖然磁場的能量在表面的導電性膜内部被當作焦耳熱 損消耗掉,但是當表面的導電性膜被研磨除去時,則其焦 耳熱損所消耗的能量係維持原樣被元件側所負擔1件内 右沒可產生渴電流的程度之導電性膜,則磁場維持原樣穿 過讀内並在外部的空間被消耗,但是在存在有某大小的 導電性膜之情況’集中地產生渦電流而引起斷線。這亦有 起因於元件的構造,但是通常當可使表面厚的導電性膜整 體產生渦電流程度之指向性高的磁場侵入元件内時,會到 處產生滿電流而造成不良影響是很清楚的。 〔0019〕 再者,在專利文獻1的方法中,係將磁場導入導電性 膜’監視其磁場所產生的渦電流量之變化以估計骐厚作 是為估計此情況膜厚,必需繼續地產生渦電流。其原因在 於,當渦電流不產生時,電路系就不動作,亦無法估計變 化的骐厚。又,研磨之結束的預測亦是,在無法估計所除 去的骐厚時,結束點或其結束點附近之亦不可能。因而, 欲監視膜厚並進行終點預測及終點檢出,必須繼續地形成 渦電流。 200912252 C 0020 ] 再者,例如,在成為研磨結束時間點附近之某既定的 殘臈量的時間點’改變研磨條件而進行處理的情況,難以 掌握是否為既定的殘膜量。可從初期膜厚之變化份量做推 測那疋因為在初期膜厚是不均的情況,既定的殘膜量的 估計會變不均的緣故。有關此研磨結束時間點附近的判 斷,當感測器與導電性薄膜間之間隙依研磨的振動而微小 地變化時’感測器電路系整體之寄生電容變化使得共振頻 率整體平移。因此,即使作了假設在成為某設定的共振頻 率時設定臨限值並判別研磨終點之設定,若共振頻率整體 平移的話,則基於其臨限值的設定之研磨結束時間點的判 斷係變得困難。 〔0021〕 如此,在習知方法中,單調且連續地增加或減少變化 的共振頻率中,就算是將臨限值設定成某I,由於感測器 與導電性_間之間隙微小地變化、或其間介設有什麼樣 的電介體,還是會有其波形自體整體地上下平行移動的情 況’其結果,預設的臨限值就沒有意義。 〔 0022〕 又,再者,於專利文獻2或專利文獻3等之方法中, 共振頻率或電阻成份輪出係直線地減少而變化,在成為择 束附近的情況,其減少的變化變和緩。但是,其變化的程 度非》常緩慢,相變得非常㈣建域餘料是哪種程度 13 〔 0023〕 200912252 又’由於磁力線係貫通元件内,因元件的構造而異’ 不僅是導電性膜,也有被形成於其他元件内的渦電流等, 所以不會有渦電流完全不流動而成為零的情況。就算完全 除去導電性膜,形成在元件内之配線等依然有部分的渦電 流流通著,因此,好像也有殘餘膜厚那樣的情況。 〔 0024〕 在使用了渦電流感測器的專利文獻2所記載的技術 中’亦將導電性膜之膜厚變化的監視,以從研磨初期到研 磨終期之渦電流的變化來觀察,和專利文獻1所記載之技 術是大致相同。 (0025) 又’在從研磨初期到研磨終期是使用渦電流而監視導 電性膜膜厚的上述習知技術中,為了在膜内引起渦電流, 有必要作出能浸透膜内的程度之夠強的磁力線,電感器的 形狀係為了使磁力線具有指向性而呈三次元形狀。因此, 在將感測器裝入研磨裝置等之後,在線圈流動的電流變大 使消粍電力變多、電源裝置變大型、且有必要將導線卷繞 成線圈狀之工程等,成本係變高。且,會發生所謂磁力線 漏洩於周邊而容易產生雜訊的問題。 〔 0026〕 專利文獻3所記載之渦電流感測器為,自研磨的初 期’磁力線貫通導電,終㈣極地㈣電流產生,而 從其滿電錢化讀取膜厚變化者,以僅產^貫通導電性 联的程度之磁場的硬體而言,無法形成渴電流而無法達成 目的又。己載有導電性膜依研磨而減少形成有渴電流 200912252 的區域係單調地減少’因此,有振盪頻率單調地減少之舉 動,把在其振盪頻率成為略一定時視為終點並檢出此部 分。亦即,此習知技術所使用之軟體的計算邏輯 (algorithm)中’振盪頻率的變化係指,把從減少到成為 略一定的變化作成振盪頻率的變化,例如,在此振堡頻率 是具有變曲點的那樣變化之情況中,終點檢出是困難。 〔 0027〕 於是’本發明之目的在於,強的磁力線不會及於導電 性膜内所形成之微細的配線,其結果係抑制由電磁誘導所 引起之渦電流的發生,並將渦電流引發的焦耳熱損抑制成 極小。 〔 0028〕 又’另一目的在於,不會有依感測器與導電性膜之間 隙的變化或研磨漿等之電介物質的介在狀態而引起渦電流 董整體平移,臨限值的設定大幅變化而變得難以檢出的事 態’即使是不貫通裝置晶圓的程度之微細的磁場,也足以 精度佳地預測/檢出研磨結束時間點,且即時算出應除去的 殘膜量及研磨率等,能正確地評估既定的導電性膜是否已 適當地除去。 〔解決課題之手段〕 〔 0029〕 本發明係為達成上述目的而提案者,申請專利範圍第 1項記載的發明提供一種研磨結束時間點之預測方法,係 在邊供給研磨级或藥液、一邊使研磨塾等之加工工具與 具有導電性骐的晶圓滑動以進行導電性膜的除去加工的研 15 200912252 磨工程中,使電感器接近晶圓上的導電性膜,監視被該電 感器所形成的磁力線引起於晶圓的導電性膜上、並依以導 電性膜的材質為一因子的集廣效應而變化的磁力線,一邊 進行晶圓面的研磨加工、一邊即時地估計研磨量 (quantities) 〇 〔 0030〕 在習知方法中,就算完全除去導電性膜,磁力線大半 是貫通元件内,所以存在於元件内的微細導電性膜,依然 流通有些§午的渴電流。因此,難以估計導電性膜完全除去 後之联厚為零的狀態’又’由於配線密度係因晶圓而異, 所以導電性膜以外的殘留渦電流之影響變得各不相同。因 而具有難以定義導電性膜是零的狀態問題。 〔 0031〕 在本發明中,因集廣效應的影響而具有急劇的變曲 點’基於此集膚效應的變曲點位置,係在未根據元件内的 狀態之下,透過表面的導電性膜之真正膜厚而幾乎被正埃 地決定成唯一。例如’很多情況是Ta膜存在於Cu膜之下, 但疋在依集膚效應而流動的電流是在極表面,且在像Cu膜 到Ta膜是導電率起大的變化之材料中’集膚效應在Cl1部 分的變化係成為受支配的,即使是Ta膜,大部分的磁場還 是未被消耗而被反射。 〔 0032〕 依本發明的方法,根據是基於集膚效應之急劇的變曲 點所顯現之特徵的磁力線變化,在各個晶圓之面内位置, 詳細地掌握膜厚變化,可即時地估計各個膜厚之不均、研 200912252 磨率、研磨形狀及均一性。 〔 0033〕 又’其特徵的磁力線變化並非以來自初期膜厚的變化 量為基準的變化。係在以完全除去的狀態為基準而殘餘骐 厚的研磨結束之前、作為急劇的變曲點加以通知。依此, 就算初期膜厚是沒有不均一的情況,亦可穩定監視殘餘膜 厚。 〔 0034〕 再者,由預先測定初期膜厚,或是由其他既測定的初 期膜厚值,檢出所即時監視的正確殘膜量,依據其結果可 算出研磨量。又,亦可從研磨的時間算出研磨率。 〔 0035〕 申請專利範圍第2項記載的發明提供一種研磨結束時 間點之預測方法,其中即時地估計上述研磨量,係殘餘膜 厚、平均膜厚、研磨形狀、研磨量、平均研磨量、研磨除 去量的不均、殘餘膜厚的不均、以及殘餘膜的形狀當中任 一者。 〔 0036〕 在本發明中,伴隨著膜厚減少’會顯現包含有依據集膚 效應的變曲點之特徵的磁力線變化,此種變化是習知技術 所無法看到的,由特徵的磁力線變化可求得殘餘膜厚平 均膜厚、研磨形狀、研磨量平均研磨量、研磨除去量的 不均、殘餘膜厚的不均、殘餘膜的形狀等。 〔0037〕 申清專利圍第3項記載的發明提供_種研磨結束時 17 200912252 間點之預測方法,其中對晶圓面一邊進行研磨加工一邊對 晶圓面内的多個部位估計研磨量。 〔 0038〕 於此發明中,此情況為,可從晶圓面内的多個部位所 各自檢出之共振頻率的波形之時間的偏差即時檢知或預測 研磨均一性。 〔 0039〕 申請專利範圍第4項記載的發明提供一種研磨結束時 間點之預測方法,其中接近上述導電性膜的電感器係二次 元平面電感器。 〔 0040〕 依據此方法,二次元平面電感器之磁場的指向性並不 尖銳,適度分散的磁場被賦與導電性膜,所以磁場難以侵 入導電性膜内,可使集膚效應的影響顯著❶因而,依據特 徵的波形,可精度佳地估計在各個位置之膜厚不均等。此 情況也與先前同樣,並非依據初期膜厚的變化,因為是依 據膜厚完全沒有的狀態之殘膜量,故能在不與初期膜厚相 依之下,穩定地求得截至結束時間點為止的殘餘膜厚。 〔0041〕 申請專利範圍第5項記載的發明提供一種研磨結束時 間點之預測方法,係在一邊供給研磨漿或藥液、一邊使研 磨墊等之加工工具與具有導電性膜的晶圓滑動以進行導電 性骐的除去加工的研磨工程中,使電感器接近晶圓上的導 電性膜,監視被該電感器所形成的磁力線引起於晶圓的導 電性臈上且依以導電性膜的㈣為—因子的集纽應而變 200912252 化的磁力線,在隨著依研磨的膜厚減少使被引起於導電性 膜的滿電流增大’且渦電流伴隨其後的膜厚減少而實質地 減少的過程中,將在導電性膜所引起之磁力線的特徵變化 之狀態換算成膜厚量,依據其相對的不均而即時地估計研 磨量。 〔 0042〕 在此方法中,由於伴隨著骐厚減少而形成的渦電流所 引起之磁力線係依集廣效應而引起特徵的變化,所以透過 監視經過其特徵變化的部分之時間,可依據其經過時間的 不均,在加工中即時地求取研磨量。 〔 0043〕 申μ專利範圍第6項記載的發明提供一種研磨結束時 間點之預測方法,係在一邊供給研磨漿或藥液、一邊使研 磨墊等之加工工具與具有導電性膜的晶圓滑動以進行導電 性膜的除去加工的研磨工程中,使電感器接近晶圓上的導 電性膜,監視被該電感器所形成的磁力線引起於晶圓的導 電性膜上且依以導電性㈣材質為―因子的集纽應而變 化的磁力線,在隨著依研磨的膜厚減少使被引起於導電性 膜的滿電流增大’ 渦電流伴隨其後的膜厚減少而實質地 減少的過程中,在晶圓面内之複數個位置求取經過其導電 性膜所引起的磁力線之特徵的變化部分時的經過時間,依 據在其複數個位置之經過時間的不均,在加工中即時地求 取研磨量® 〔 0044〕 依本發明’除了申請專利範圍第5項記載的發明之作 200912252 用以外,透過在晶圓面内之複數個位置,監視經過其特徵 的變化之部分的時間,可依據其經過時間的不均,即時地 求取全面的研磨量。 〔 0045〕 申請專利範圍第7項記載的發明提供一種研磨結束時 間點之預測方法,係在一邊供給研磨漿或藥液、一邊使研 磨墊等之加工工具與具有導電性膜的晶圓滑動以進行導電 性膜的除去加工的研磨工程中,使電感器在相對於晶圓不 同的軌跡位置上作複數配置並接近晶圓,監視利用由該電 感器所形成的磁力線而在既定的晶圓面内之複數個位置所 引起於導電性骐之磁力線變化,依據上述導電性膜的集廣 效應,在晶圓面内之複數個位置求取經過其導電性膜所引 起的磁力線之特徵的變化部分時之經過時間,換算成研磨 除去量的不均,抑或從波形的變化率換算複數個位置之各 個膜厚量,依據其不均或膜厚量,在加工中即時地求取研 磨量。 〔 0046〕 在此方法中,藉由從經過引起於導電性膜之特徵的磁 力線變化的部分時的經過時間,求取研磨除去量的不均或 在複數個位置之各個膜厚量,可精度佳地監視研磨量。 〔 0047〕 申請專利範圍第8項記載的發明提供一種研磨結束時 間點之預測方法,其中依據上述導電性犋之集膺效應所引 起之磁力線變化的測定手段,係導電性骐中的渦電流之測 定,或,透過導電性膜產生渦電流而產生的互感之測定, 20 200912252 或,基於導電性膜之互感的上述電感器之感測器電路系中 的電感變化之測定,或,感測器電路系的阻抗變化之測定, 或使該感測器電路系的電感變化與高頻電感器和電容並聯 連接並使之振盪而測定其共振頻率之測定當中至少任一 者。 〔 0048〕 在本發明的預測方法中,伴隨著膜厚減少會顯現含有 依據集膚效應的變曲點之特徵的磁力線變化,這樣的變化 是習知技術所未見的,所以透過基於磁力線變化的各種 數值(渦電流、互感、阻抗變化等)可預測研磨量。 〔 0049〕 以下叙述以上所述之申請專利範圍第1項至第8項所 記載之本發明與習知技術之相異點。首先,在本發明中, 並非於膜内積極地誘發渦電流以進行骐厚的計測者。乃利 用導體膜對磁場之集膚效應,極力阻止磁場朝導電性膜侵 入,在膜厚除去附近檢知因一部份磁場自導體膜漏出所產 生的’/尚電流’再由其變化形態來預測結束點者β 〔 0050〕 又,極力減輕依表面的導電性膜產生的渦電流而造成 存在於其導電性膜下的元件之部分所消耗的磁場能量。在 導電性膜被除去之前,伴隨著膜厚減少使總渦電流逐漸減 少的過程中’由於磁場的能量對内部的元件造成影饗,所 以作成極力防止磁場朝元件内部侵入以減輕磁場的能量。 〔0051〕 於專利文獻2中,檢出導電性膜骐厚用的感測器線 21 200912252 圈,具備有與信號源連接的振盪線圈、配置於振盪線圈的 導電性膜側之檢出線圈、以及配置在振盪線圈之導電性膜 側的相反側之平衡線圈,且將可變電阻以檢出線圈和平衡 線圈相互形成反相的方式作連接的串聯電路連接,在未存 在有屬檢出對象的導電性膜時,可調整成前述串聯電路的 輸出為零,從以檢出電路檢出的電阻成份及電抗成份輸出 合成阻抗,再由合成阻抗的變化將導電性膜的膜厚變化, 在寬廣的範圍中當成大約直線關係來進行檢出。 〔 0052〕 但是’在本發明中,作為電感器,不必要是振盪線圈、 檢出線圏、及平衡線圈3個線圈。且,並非將其線圈以立 體方式作3次元層疊以監視其磁力線變化者。而是只有一 個成為電感器的線圏,且建構成2次元平面者。 〔 0053〕 又,在專利文獻2中,是作成將可變電阻連接到使檢 出線圏和平衡線圏相互呈反逆地連接的串聯電路,但本發 明中’可變電阻等之電阻並不是挾的。本發明的振盪電路 係將電容對電感器並聯結合者。 〔 0054〕 又’依據上述公報,膜厚變化從電阻成份和電抗成份 輸出合成阻抗,此合成阻抗係對膜厚變化在寬廣的範圍形 成略直線的關係,從其直線的變化關係求取膜厚。但是, 在本發明中’並非以在寬廣的範圍中測定膜厚為目的。係 在研磨結束時間點之前依據特徵的波形之變化而正確地預 測研磨結束點者。 22 200912252 〔 0055〕 又’在其研磨結束時間點之前之特徵的波形之變化並 不是略直線的變化。係依集膚效應之影響而具有急劇的變 曲點’依據其變曲點及其前後之急劇的變化率等之特徵點 而正確地預測研磨結束時間點者。 〔 0056〕 又’依據上述公報’在段落0027中係在圓7 (b)中 不出相對於導電性膜膜厚之變化的電阻份量之變化(附件 一)。電阻份量的變化對祺厚變化之關係為,隨著骐厚從厚 變薄之變化,電阻份量R係如圖面般地變化。亦即,在極 薄膜厚之區域(a)中’電阻份量R的輸出係呈直線地大變 化,當成為某厚度之區域(b)時,電阻份量R的變化飽和, 接著在膜厚變厚的區域(c) +,電阻份量R的輸出降低。 在此,於銅膜的情況,(a)點表示約1〇〇〇 λ左右,(b) 點表示2000 A〜3000A,(c)點表示5〇〇〇A以上。 〔 0057〕 但疋’像導電性膜厚之電阻份量係依膜厚而變大、之 後再變小那樣的舉動乃顯示出圓的軌跡係在電阻成份和 電k成f”之平衡巾從其相位相互重4而來的,並非像本發 明是依據集廣效應者,舉動完全不同。 〔 0058〕 在本發明中’依集廣效應,從磁力線不侵入導電性骐 内的過程’—部份_力線隨著膜厚減少而漏,之後, 在磁力線貫通某程度時,透過所謂滿電流會對應膜的趙積 而減)之基於—連串的集廣效應之減少,急劇的變曲點係 23 200912252 被產生。其變曲點並非單純僅影響頻率者。如同後面所示 之改變電感器距離和電感器直徑而棋擬的事例所示,即便 是相同頻率’還是會有因電感器的直徑或電感器與導電性 膜之距離使磁場的指向性改變,磁場朝導電性膜内侵入舉 動起大變化的情況。以某電感器直徑和電感器距離而言, 在研磨時的膜厚減少之過程具有基於集膚效應的變曲點, 但以例如1/1000的電感器大小和電感器距離而言,在研 磨時的膜厚減少的過程中,存在著未具有基於集廣效應的 變曲點之情況。此乃清楚表示,並不僅是那時的頻率在 電感器形狀或距離等之設定中,磁場的指向性變化,依集 膚效應,磁場對導電性膜之侵入特性變化,變曲點的狀態 變化。 4 〔 0059〕 本發明中,把從磁場未朝這樣的導電性膜内侵入的狀態 到持續侵入的狀態中之現象的變化過程,形成利用研磨使 膜厚減少的過程,利用其狀態變化而精度佳地預測導電性 膜被除去的點者。 〔 0060〕 如此’本發明中依據集廣效應之電阻成份的變化,與 從習知技術之電阻成份與電抗成份之相位關係所求之電阻 成份的變化係完全不同的。 〔0061 〕 又’依據專利文獻3(專利第3902064號公報),首先, 在先行技術的段落〇〇 12,於依據習知的渦電流感測器之研 磨終點的檢出方法中,由於渦電流感測器所使用的振盪頻 24 200912252 率是較小的7Μ1ΪΖ左右,所以在研磨對象之導電性骐是相當 厚的情況,雖可檢出大的渦電流損,但是當導電性膜的研 磨進行使膜厚變極薄時,渦電流損的大小變小,在此情況, 例如1000 A以下程度的膜厚檢出係變得困難β亦即,習知 的/尚電流感測器因為振盛頻率較低,所以在要求是埃等級 之膜厚檢出精度的研磨裝置之研磨終點的檢出上,具有所 謂其精度不足的問題。 〔 0062〕 而且揭示著,不論是厚的膜厚或是薄的膜厚同樣可使 磁場侵人膜内,依其磁場所引起㈣電流大小來單純地監 視膜厚的方法。 〔 0063〕 但是,在本發明中並未將導電性膜較厚的情況當作問 題反疋纟導電性膜厚的情況,磁場係依集廣效應而 不侵入於導電㈣内,因此被要求不檢出大的满電流。又, 在膜厚逐漸減少到刪Α程度之情況,即使是無指向性的 磁場’由於貫通-部份導電性❹隨著料的減少形成满 :流並生成斥力磁場,所以亦可對其精度佳地檢出。係把 性職除去之前附近的集歧應之㈣的舉動結 度佳地預測研磨結束時間點者,並非以即使 疋厚的膜厚也進行膜厚測定為目的者。 〔 0064〕 的振通頻率作號掌握作為頻:,係將滿電流感測器 之時門气八, &頻率的時間梯度並演算振盪頻率 ‘錢,依此特徵點來進行研磨終點的判定。圖 25 200912252 5 ( a)係顯示振盘頻率自想 目猫之時間t的推移轨跡,圓5 (b)係顯示此微分值之推移軌跡(附件。 〔 0065〕 此振盈頻率之舉動係示出振i頻率單調地減少的舉 動丄在此振盡頻率之單調減少點的最下點進行研磨終點之 判定者X,透過微分其波形而找出翠調減少中之變化點 以判定為終點。 ^ 〔 0066〕 但是,以本發明而言,這樣的振逢頻率之舉動係不同。 亦即,本發明中在利用研磨減少膜厚之過程,振盡頻率係 依導電性膜之集膚效應而隨著膜厚減少而暫時上昇,之後 再下降,在接近終點處具有一個峰值。此舉動乃係依集膚 效應使磁場從不侵人直到侵人於導電性膜内的過程而產生 者,與先前的公知例所示的舉動明顯有異。 〔 0067〕 而且,本發明係檢出上昇並下降的變曲點以及其變曲 點附近之特徵的部分,而精度佳地預測研磨之結束時間點。 〔 0068〕 又,在專利文獻3中,渦卷狀的感測器線圈被配置成 與基板正交,但相對地,在本發明中的線圏,係以與基板 平行的形態配置一個平面電感器,在裝置的構成點上也明 顯不同^ 〔 0069〕 再者’在專利文獻3中’如段落〇〇32所示,係顯示電 阻成份隨著膜厚減少而一次增大、之後再減少的舉動。但 26 200912252 是’此乃非依集廣效應而顯現的舉動。在圊面所示的電路 中’在其相位差中由電阻成份和電抗成份之平衡所產生的 變曲點。亦即’本發明中的變曲點係與這樣的變曲點完全 不同。如同先前所述’變曲點係依線圈的大小、形狀、或 導電性膜到線圈的距離而發生大的變化,依其設定,亦存 在有即使是高頻帶也無法看見依據集膚效應之特徵的舉動 之情況。 〔 0070〕 在本發明中,適當地設定其導電性膜的導電率、透磁 率及頻率、電感器形狀以及電感器和導電性薄膜之距離 等,在利用研磨使膜厚減少的過程中,作為振盪頻率依集 膚效應而具有變曲點的狀態’依據其波形之特徵的部分, 精度佳地預測研磨結束時間點者。 〔發明效果〕 〔0071〕 圓上的導電性膜,監視依導電性膜的f/ϊ效應而變化的域 ’係使電感器接近晶200912252 IX. Description of the Invention: [Technical Field] [0001] The present invention relates to a method for predicting a polishing end time point when polishing a conductive yt formed on a semiconductor wafer, in particular, In the inductor, a change in the characteristics of the oscillation frequency of the conductive film is detected, and a method of predicting the polishing state and the polishing end time point at which the polishing end time is predicted is detected. [Prior Art] [0002] It is understood that the process is such that an oxide film is formed on the surface of the semiconductor wafer, and a groove pattern corresponding to the wiring pattern is formed on the oxygen "needle plate (i) iKmhQgraphy) and (4), and then a film is formed thereon. There is a conductive film made of Cu or the like which is filled with a groove pattern, and the unnecessary portion other than the buried portion such as the groove pattern or the through hole portion in the conductive film is removed by chemical mechanical polishing. Wiring pattern. With the formation of the case, it is important to detect the conduction of the unnecessary portion, and it is important to remove the polishing end and to stop the process when the thickness is appropriately removed. When the electrical film is overgrown, the resistance of the wiring is increased, and when the polishing is too small, the wiring insulation is hindered. [0003] In the conventional art relating to the monitoring method of the grinding state, for example, Patent Document 1 discloses a method of monitoring the change in the thickness of the film on the spot. In the method of removing the conductive film from the substrate (the semi-conductive Zhao Jingyuan) by chemical mechanical polishing, the method of monitoring the thickness variation of the conductive film on the spot is made to contain iron. Oxygen tank type line 200912252 感 The sensor of the resonant circuit in series or parallel connection between the inductor and the capacitor is arranged close to the conductive film, and the scan output from the high frequency excitation signal source is set through the operating point. Applying 'by this' to the sensor by means of impedance means that when the sensor is energized, the oscillating current flows in the coil, creating an alternating electromagnetic field. This alternate electromagnetic field then induces a thirsty current in the conductive film. When the eddy current is induced to the conductive film, two effects are produced. First, the conductive film acts as a loss resistor, and the effect is on the resistance load of the sensing circuit, which lowers the amplitude of the resonance signal and lowers the resonance frequency. Second, when the thickness of the electroconductive thin film is reduced, the same effect as the metal rod disposed at the center of the coil of the inductor is extracted, thereby causing a change in inductance and a frequency shift. By continuously monitoring the frequency shift associated with the resonance peak of the sensor due to the thickness variation of the conductive film, the thickness variation of the conductive film is continuously detected. [0004] Further, other conventional technical aspects are known. There is an eddy current sensor as described below (Patent Document 2). Patent Document 2 is a prior art in which a eddy current is formed by a conductive film provided on a surface of a semiconductor substrate, and an eddy current sensor indirectly performs measurement of a film thickness in accordance with the eddy current. It is difficult to perform the problem of correct thickness detection (segment S GGG4)', and it is possible to provide a film thickness from a very thin film thickness formed on a semiconductor substrate to a thick conductive film. For the purpose of detecting the thirst current sensor (paragraph 0005) » [0005] Thus, in this document, there is a sensing coil disposed near a conductive film or a substrate having a conductive film of 200912252 (vortex) a current sensor) for supplying an alternating current signal of a certain frequency to the sensing coil to form an alternating current signal source for eddy current on the conductive film, and a detecting circuit for measuring a reactance component and a resistance component including the conductive film. The sensing coil includes an oscillation coil connected to the signal source, a detection coil disposed on the conductive film side of the oscillation coil, and a flat surface disposed on the opposite side of the conductive film side of the oscillation coil. Coil 'and so as to balance coil and the detection coil as a mutual connection for the inverter. Then, the resistance component and the reactance component detected by the detection circuit output a combined impedance, and the change in impedance is used to detect the film thickness variation of the conductive film in a wide range as a linear relationship. [0006] In the case of Patent Document 2, for example, an eddy current is generated in a thick film and the film thickness is measured. On the other hand, when the thick film is polished to reduce the amount of eddy current, the eddy current is reduced. Among the reduced components, the energy of the magnetic field is not simply consumed by the conductive film on the surface, and remains as it is inside the element below the conductive film, that is, the energy of the magnetic field that would otherwise be consumed in the conductive film. As the conductive film is removed, the inside of the element is allowed to be exposed to the energy of the excess magnetic field. [0007] Further, regarding other conventional techniques, for example, a thirst current sensor (Patent Document 3) is known. First, as a prior art, in paragraph (0012), the detection method of the polishing end point of the conventional eddy current sensor is that the oscillation frequency used in the eddy current sensor is about 7 MHz, which is small, so When the conductive film to be polished is thick enough, a large eddy current loss of 200912252 can be detected. However, when the polishing of the conductive film is performed and the film thickness is extremely thin, the magnitude of the eddy current loss is small, which is difficult in this case. A film thickness of, for example, 丨〇〇〇a or less is detected. In other words, the conventional eddy current sensor has a problem that the accuracy is insufficient in the detection of the polishing end of the polishing apparatus which is required to have the film thickness detection accuracy of the angstrom level because of the low oscillation frequency. [0008] Here, a method of simply monitoring the film thickness based on the magnitude of the eddy current of the magnetic field in the same manner regardless of the thickness of the film or the thickness of the film is disclosed. The technique of Patent Document 3 also changes the magnetic field lines formed by the sensor coils through the conductive film disposed on the entire substrate of the sensor coils, and alternately changes, as in the prior art. The eddy current is generated in the conductive film, and the eddy current is transmitted through the conductive film. The eddy current loss occurs in the middle of circulation, and the reactance component of the impedance of the sensor coil is reduced by the equivalent circuit (paragraph 〇008) β [0009], and the change of the oscillation frequency of the oscillation circuit is observed, accompanied by When the polishing is performed, when the conductive film is thinned, the oscillation frequency is lowered accordingly. When the conductive film is completely absent due to polishing, it becomes the oscillation frequency of the groove circuit itself, and after that, the oscillation frequency is slightly fixed. Therefore, by detecting this point, the end point of the chemical mechanical polishing of the conductive film can be detected (paragraph 0009). [0010] Further, as shown in Fig. 2 of the document, when the polishing of the conductive film is performed, the eddy current loss changes, and the equivalent resistance value of the sensor turns changes. Therefore, since the oscillation frequency of the oscillating circuit changes, the frequency-dividing signal is divided by the frequency-dividing circuit through the 12112252, or the subtraction is performed by the subtractor, and the signal corresponding to the frequency of the detected width is displayed on the monitoring. Device. Thereby, the transition of the frequency trajectory as shown in Fig. 2 (segment 0025) can be obtained. C 0011) Further, an eddy current sensor such as the following is known (Patent Document 4). In this document, please patent the brain! A full-current sensor is provided with a sensor coil disposed near a substrate on which a conductive film is formed, and an alternating current signal is supplied to the sensor coil to form an eddy current source in the conductive film. And a detection circuit for detecting an eddy current formed on the conductive film as an impedance seen by the sensor coil, wherein the full current sensor is characterized in that the sensor line is modified by a high permeability The inside of the receiving member formed by the magnetic material. [0012] Further, in the seventh application of the document, an eddy current sensor is disclosed which is provided with a sensor coil disposed adjacent to a substrate on which a conductive film or a conductive film is formed, The sensor coil supplies an AC signal, and a signal source for forming an eddy current in the conductive film and a detection circuit for detecting an eddy current formed in the conductive film as an impedance seen by the sensor coil. The eddy current sensor is characterized in that the resistance component and the reactance component of the impedance are displayed on a right coordinate axis, and the conductive is detected from an angle formed by a line connecting a coordinate of the impedance to a coordinate of a specified center point. The film thickness of the film. [Patent Document 1] Patent No. 2878178 (page 2 to page 7) Figs. 1 to 15). [Patent Document 2] Patent No. 3587822 (Page 3, FIG. 1 to FIG. 11) 专利 [Patent Document 3] Patent No. 39〇2〇64 (Patent Document 4) JP-A-2005-121616 [Invention [Problem to be Solved by the Invention] [0013] In the method for monitoring the thickness of the film of Patent Document 1, the sensor is used in a coil of a ferrite tank type which is wound in a directivity for making an electromagnetic field. A series or parallel resonant circuit of the inductor and the capacitor. Next, in the initial stage of grinding, 20Hz~40. The scanning output of the frequency of 1 MHz is applied to the sensor, and the alternating electromagnetic field having directivity generated by the coil generates a leakage magnetic field line that penetrates the conductivity and is induced from the initial stage of the polishing. The film thickness corresponds to a large thirst current. [0014] In order to induce a large thirst current corresponding to the film thickness of the conductive film, a large alternating electromagnetic field, that is, a magnetic field line which is large enough to penetrate the conductive film, is required, and the thickness of the conductive film changes. The monitoring system is carried out using a thirst current caused by the polishing oil to the end of the polishing and the thinness of the conductivity. Therefore, it is necessary to pass the magnetic lines of force toward the thickness direction of the conductive film while monitoring the change in thickness. In the drawings of the patent document, the magnetic lines of force penetrating through the conductive film described in the entire portion of the conductive film are clear. [0015] 10 200912252 On the surface of the wafer at the initial stage of polishing, a generally non-scaling Cu film (conductive film) is located on the uppermost layer. In order to induce a full current on all of the scale-free Cu films, a very large leak magnetic field line is required. However, although the leakage magnetic field lines can induce eddy currents, they are all consumed as Joule heat in the form of so-called eddy current loss. This "Joule heat loss, for the most surface-free non-scaling Cu film, due to the small volume resistance, the heat is relatively low. The part which is small and has been internally wired has a small cross-sectional area and a large volume resistance, so that a large eddy current is induced by the magnetic lines of penetration, and as a result, a large Joule heat loss is locally generated. This occasion will develop into a part of the problem of wiring melting and disconnection. It becomes a state of so-called induction heating, which is particularly a phenomenon of causing sweltering inside. In particular, in the case of Cu wiring or the like, there is a case where Cu is heated to diffuse on the blocking film of Ta or the like after Cu is heated, or it may be caused by the breakthrough of the blocking film due to the occasion. [0016] In the case where a plurality of layers of wiring are applied to the surface portion of the wafer, not only the Cu film on the surface layer but also the wiring portion inside the processed portion may be partially warmed. Diffusion into the surrounding, or formation of P-type, n-type dopants in the semiconductor substrate and then diffuse and change the characteristics of the components in the substrate. Further, even when heat is not generated, when excessive eddy current is caused to flow through the fine wiring, electromigration may occur to cause disconnection. [0017] Damage to the component caused by the magnetic field invading the component can be explained as follows. In other words, in the method of Patent Document 1, an eddy current is formed in a portion of the conductive film (Cu film) on the surface in accordance with the invading magnetic field, and a repulsive magnetic field is generated depending on the eddy current. At the initial stage of the polishing, since the conductive film 200912252 J that passes through the covering surface prevents the magnetic field from entering the internal element, damage to the element is small. On the energy surface: the eddy current generated by the conductive film covering the surface is consumed as a Joule heat in the conductive film. Therefore, at the initial stage of the grinding, the internal components are protected from the partial magnetic field by the conductive film on the surface. [0018] However, when the polishing is performed to remove the film of the conductive film covering the surface, the magnetic field intrudes into the element without being alleviated. In the initial stage of polishing, although the energy of the magnetic field is consumed as Joule heat loss inside the conductive film on the surface, when the conductive film on the surface is removed by grinding, the energy consumed by the Joule heat loss is maintained as it is. When the conductive film of the extent that no thirst current is generated on the right side of the component side, the magnetic field remains as it is and is consumed in the external space, but in the presence of a conductive film of a certain size The ground generates eddy currents and causes disconnection. This is also caused by the structure of the element. However, when a magnetic field having a high directivity of the eddy current is intruded into the element by a conductive film having a thick surface as a whole, it is clear that a full current is generated everywhere and the adverse effect is caused. [0019] Further, in the method of Patent Document 1, a magnetic field is introduced into the conductive film to monitor the change in the amount of eddy current generated by the magnetic field to estimate the thickness of the film, in order to estimate the film thickness in this case, it is necessary to continue to generate Eddy current. The reason is that when the eddy current is not generated, the circuit system does not operate, and it is impossible to estimate the thickness of the change. Further, the prediction of the end of the polishing is also impossible, when it is impossible to estimate the thickness of the removed, the end point or the vicinity of the end point thereof is impossible. Therefore, in order to monitor the film thickness and perform end point prediction and end point detection, it is necessary to continuously form an eddy current. In the case where the polishing conditions are changed and the processing is performed at a time point of a predetermined amount of the residue near the polishing completion time point, it is difficult to grasp whether or not the predetermined residual film amount is present. It is possible to estimate from the change in the initial film thickness. Since the film thickness is uneven at the initial stage, the estimated amount of residual film may become uneven. Regarding the judgment near the polishing end time point, when the gap between the sensor and the electroconductive thin film slightly changes depending on the vibration of the polishing, the parasitic capacitance change of the entire sensor circuit system causes the resonance frequency to shift as a whole. Therefore, even if it is assumed that the threshold value is set and the setting of the polishing end point is determined when the resonance frequency is set, if the resonance frequency is shifted as a whole, the determination of the polishing end time point based on the setting of the threshold value becomes difficult. [0021] Thus, in the conventional method, in the monotonously and continuously increasing or decreasing the varying resonant frequency, even if the threshold is set to a certain value I, the gap between the sensor and the conductivity _ is slightly changed, Or what kind of dielectric is interposed between them, or there will be a case where the waveform itself moves up and down in parallel as a whole. As a result, the preset threshold does not make sense. Further, in the method of Patent Document 2 or Patent Document 3, the resonance frequency or the resistance component wheeling linearly decreases and changes, and when it is in the vicinity of the selection, the change in the decrease becomes gentle. However, the degree of change is not always slow, and the phase becomes very (4). What is the extent of the remaining material? 13 [ 0023] 200912252 And 'because magnetic lines are penetrated into the component, depending on the structure of the component' is not only a conductive film. There are also eddy currents or the like formed in other elements, so there is no case where the eddy current does not flow at all and becomes zero. Even if the conductive film is completely removed, a part of the eddy current flows through the wiring or the like formed in the element. Therefore, there is a case where the residual film thickness is also present. [0024] In the technique described in Patent Document 2 using an eddy current sensor, the monitoring of the change in the thickness of the conductive film is also observed, and the eddy current is observed from the initial stage of polishing to the end of polishing, and the patent The technique described in Document 1 is substantially the same. (0025) Further, in the above-described conventional technique for monitoring the thickness of the conductive film using an eddy current from the initial stage of polishing to the end of polishing, in order to cause an eddy current in the film, it is necessary to make it sufficiently strong to penetrate the film. The magnetic lines of force, the shape of the inductor is a three-dimensional shape in order to make the magnetic lines of force have directivity. Therefore, after the sensor is placed in the polishing apparatus or the like, the current flowing through the coil is increased, the power consumption of the power is increased, the power supply device is enlarged, and the wire is wound into a coil shape, and the cost is high. . Further, there is a problem that magnetic flux leaks to the periphery and noise is likely to occur. [0026] The eddy current sensor described in Patent Document 3 is that since the initial stage of the polishing, the magnetic field lines are electrically conductive, and the final (fourth) polar (four) current is generated, and the film thickness is changed from the full charge, and only the product is produced. In the hardware of a magnetic field that penetrates the degree of conductivity, a thirsty current cannot be formed and the object cannot be achieved. The region in which the conductive film is loaded and reduced to form the thirsty current 200912252 is monotonously reduced. Therefore, there is a behavior in which the oscillation frequency monotonously decreases, and the oscillation frequency is regarded as an end point and the portion is detected as the end point. . That is, the variation of the oscillation frequency in the calculation logic of the software used in the prior art refers to the change of the oscillation frequency from the decrease to the slightly certain change, for example, the vibration frequency of the vibration is In the case of a change in the point of change, it is difficult to detect the end point. [0272] Thus, the object of the present invention is that a strong magnetic line of force does not conform to the fine wiring formed in the conductive film, and as a result, the occurrence of eddy current caused by electromagnetic induction is suppressed, and the eddy current is induced. Joule heat loss is suppressed to a minimum. [0028] Another purpose is that there is no change in the gap between the sensor and the conductive film or the interposition of the dielectric substance such as the slurry, and the eddy current is totally shifted. The situation that becomes difficult to detect is changed. Even a fine magnetic field that does not penetrate the wafer of the device is sufficient to accurately predict/detect the polishing end time point, and instantly calculate the amount of residual film and the polishing rate to be removed. Etc., it is possible to correctly evaluate whether or not a predetermined conductive film has been properly removed. [Means for Solving the Problem] [0029] The present invention has been made in order to achieve the above object, and the invention according to the first aspect of the invention provides a method for predicting the end time of polishing, which is to supply a polishing stage or a chemical solution. In the grinding process, the processing tool such as the polishing crucible and the wafer having the conductive crucible are slid to perform the removal process of the conductive film. In the grinding process, the inductor is brought close to the conductive film on the wafer, and the inductor is monitored by the inductor. The magnetic lines of force are formed on the conductive film of the wafer, and the magnetic fluxes which change according to the broadening effect of the material of the conductive film are subjected to the polishing process of the wafer surface, and the amount of grinding is estimated instantaneously. 〇 [ 0030] In the conventional method, even if the conductive film is completely removed, most of the magnetic lines of force penetrate through the element, so that the fine conductive film existing in the element still flows a little **** noon current. Therefore, it is difficult to estimate a state in which the thickness of the conductive film after the complete removal of the conductive film is zero. In addition, since the wiring density varies depending on the wafer, the influence of the residual eddy current other than the conductive film is different. Therefore, it is difficult to define a state in which the conductive film is zero. [0031] In the present invention, there is a sharp inflection point due to the effect of the collective effect, and the position of the inflection point based on the skin effect is a conductive film that passes through the surface without being in the state of the element. The true film thickness is almost uniquely determined by the positive. For example, 'in many cases, the Ta film exists under the Cu film, but the current flowing in the skin effect according to the skin effect is on the surface of the pole, and in the material such as the Cu film to the Ta film which is a large change in conductivity. The effect of the skin effect on the Cl1 portion is dominated. Even with the Ta film, most of the magnetic field is not consumed and is reflected. [0032] According to the method of the present invention, the change in the thickness of the film is obtained in detail in the in-plane position of each wafer based on the change in the magnetic field lines characteristic of the sharp inflection point of the skin effect, and the respective thicknesses can be estimated in real time. Uneven film thickness, grinding 200912252 grinding rate, grinding shape and uniformity. [0033] Further, the change in magnetic field lines characteristic of the change is not based on the amount of change from the initial film thickness. It is notified as a sharp inflection point before the end of the polishing in which the residual thickness is based on the state of complete removal. Accordingly, even if the initial film thickness is not uneven, the residual film thickness can be stably monitored. [0034] Further, the amount of the correct residual film to be immediately monitored is detected by measuring the initial film thickness in advance or by the other initial film thickness values measured, and the amount of polishing can be calculated based on the result. Moreover, the polishing rate can also be calculated from the polishing time. [0035] The invention according to claim 2 provides a method for predicting a polishing end time point, wherein the polishing amount is estimated instantaneously, which is a residual film thickness, an average film thickness, a polishing shape, a polishing amount, an average polishing amount, and a grinding. Any of the unevenness of the removal amount, the unevenness of the residual film thickness, and the shape of the residual film. [0036] In the present invention, as the film thickness decreases, a change in the magnetic field line including the characteristic of the inflection point according to the skin effect is exhibited, which is not seen by the prior art and is changed by the characteristic magnetic field line. The residual film thickness average film thickness, the polishing shape, the polishing amount average polishing amount, the unevenness of the polishing removal amount, the variation of the residual film thickness, the shape of the residual film, and the like can be obtained. [0037] The invention described in the third paragraph of the Japanese Patent Laid-Open No. 3 provides a method for predicting the point between the end of the polishing and the 17 200912252, wherein the polishing amount is estimated for a plurality of portions in the wafer surface while polishing the wafer surface. [0038] In the present invention, in this case, the polishing uniformity can be immediately detected or predicted from the time difference of the waveform of the resonance frequency detected by each of the plurality of portions in the wafer surface. [0039] The invention of claim 4 provides a method of predicting a polishing end time point in which an inductor-based secondary element planar inductor is adjacent to the conductive film. [0040] According to this method, the directivity of the magnetic field of the quadratic planar inductor is not sharp, and the magnetic field which is moderately dispersed is imparted to the conductive film, so that it is difficult for the magnetic field to intrude into the conductive film, and the effect of the skin effect is remarkable. Therefore, according to the waveform of the feature, the film thickness unevenness at each position can be accurately estimated. In the same manner as before, the change in the initial film thickness is not based on the amount of residual film in a state in which the film thickness is completely absent, so that the end time can be stably obtained without depending on the initial film thickness. Residual film thickness. [0041] The invention according to claim 5 provides a method for predicting a polishing completion time point by sliding a processing tool such as a polishing pad and a wafer having a conductive film while supplying a polishing slurry or a chemical solution. In the polishing process for removing the conductive germanium, the inductor is brought close to the conductive film on the wafer, and the magnetic field lines formed by the inductor are monitored to cause conductivity on the wafer and the conductive film is used. The magnetic field line of the 200912252 is reduced by the decrease of the film thickness according to the polishing, and the full current of the conductive film is increased, and the eddy current is substantially reduced with the subsequent film thickness reduction. In the process, the state of the characteristic change of the magnetic lines of force caused by the conductive film is converted into the film thickness, and the amount of polishing is immediately estimated based on the relative unevenness. [0042] In this method, since the magnetic field lines caused by the eddy current formed by the reduction of the thickness of the crucible cause a characteristic change due to the collective effect, the time for monitoring the portion passing through the characteristic change can be followed by Time is uneven, and the amount of grinding is instantaneously obtained during processing. [0043] The invention according to claim 6 of the present invention provides a method for predicting a polishing end time point, in which a processing tool such as a polishing pad and a wafer having a conductive film are slid while supplying a polishing slurry or a chemical liquid. In the polishing process for removing the conductive film, the inductor is brought close to the conductive film on the wafer, and the magnetic lines of force formed by the inductor are monitored on the conductive film of the wafer and the conductive (four) material is used. The magnetic field lines that change according to the "factor" of the factor are caused by the decrease in the film thickness due to the polishing, which causes the full current of the conductive film to increase, and the eddy current is substantially reduced as the film thickness thereafter decreases. The elapsed time when the change portion of the characteristic of the magnetic field line caused by the conductive film is obtained at a plurality of positions in the plane of the wafer, and is instantaneously obtained in the processing according to the unevenness of the elapsed time at the plurality of positions The amount of grinding is taken [0044] According to the invention of the present invention, except for the use of the invention 200912252 described in claim 5, the monitoring is carried out through a plurality of positions in the plane of the wafer. Part of the time change of its characteristics, which can be based on elapsed time uneven, instantly strike a comprehensive amount of grinding. [0045] The invention according to claim 7 provides a method for predicting a polishing end time point by sliding a processing tool such as a polishing pad and a wafer having a conductive film while supplying a polishing slurry or a chemical solution. In the polishing process for removing the conductive film, the inductor is placed in a plurality of different track positions with respect to the wafer and is close to the wafer, and the magnetic field lines formed by the inductor are used to monitor the predetermined wafer surface. The magnetic field lines of the conductive defects caused by the plurality of positions in the plurality of positions, and the change portions of the magnetic lines of force caused by the conductive film are obtained at a plurality of positions in the wafer surface according to the collective effect of the conductive film The elapsed time is converted into the unevenness of the amount of polishing removal, or the amount of each film thickness at a plurality of positions is converted from the rate of change of the waveform, and the amount of polishing is immediately obtained during processing based on the unevenness or the amount of film thickness. [0046] In this method, the unevenness of the amount of polishing removal or the thickness of each film at a plurality of positions can be obtained by the elapsed time from the portion where the magnetic field lines which are characteristic of the conductive film are changed, and the precision can be obtained. Good to monitor the amount of grinding. [0047] The invention according to claim 8 provides a method for predicting a polishing end time point, wherein the measuring means of the magnetic field line change caused by the set effect of the conductive enthalpy is an eddy current in the conductive crucible Measuring or measuring the mutual inductance generated by the eddy current generated by the conductive film, 20 200912252 or measuring the change in inductance in the sensor circuit of the inductor based on the mutual inductance of the conductive film, or the sensor The impedance change of the circuit system is measured, or at least one of the measurement of the resonance frequency of the sensor circuit is measured by connecting the high frequency inductor and the capacitor in parallel and oscillating. [0048] In the prediction method of the present invention, as the film thickness decreases, changes in magnetic lines of force including characteristics of the inflection point according to the skin effect appear, which are not seen in the prior art, so that the change is based on the magnetic line of force. Various values (eddy current, mutual inductance, impedance change, etc.) can predict the amount of grinding. [0049] The difference between the present invention described in the first to eighth aspects of the above-mentioned patent application scope and the prior art is described below. First, in the present invention, it is not a measure that positively induces eddy currents in the film to perform thickness measurement. The effect of the skin effect of the conductor film on the magnetic field is to prevent the magnetic field from invading into the conductive film. In the vicinity of the film thickness removal, it is detected that a part of the magnetic field leaks from the conductor film and then changes its shape. The predicted end point β [0050] Further, the eddy current generated by the conductive film on the surface is reduced as much as possible to cause the magnetic field energy consumed by the portion of the element existing under the conductive film. Before the conductive film is removed, the total eddy current is gradually reduced as the film thickness is reduced. Since the energy of the magnetic field affects the internal components, it is possible to prevent the magnetic field from entering the inside of the element to reduce the energy of the magnetic field. [0021] In Patent Document 2, the sensor line 21 200912252 is used for detecting the thickness of the conductive film, and includes an oscillation coil connected to the signal source, a detection coil disposed on the conductive film side of the oscillation coil, and And a balance coil disposed on the opposite side of the conductive film side of the oscillating coil, and the varistor is connected in a series circuit in which the detecting coil and the balanced coil are connected to each other in an inverted manner, and there is no detected object In the case of the conductive film, the output of the series circuit can be adjusted to zero, the combined resistance is outputted from the resistance component and the reactance component detected by the detection circuit, and the film thickness of the conductive film is changed by the change of the combined impedance. In a wide range, it is detected as a linear relationship. [0052] However, in the present invention, as the inductor, it is not necessary to have three coils of the oscillation coil, the detection coil, and the balance coil. Moreover, the coils are not stacked in a three-dimensional manner in a stereoscopic manner to monitor changes in their magnetic lines. Instead, there is only one turn that becomes the inductor, and it is constructed as a 2-dimensional plane. Further, in Patent Document 2, a series circuit in which the variable resistor is connected to the detection coil and the balance coil 反 is connected in reverse, but in the present invention, the resistance of the variable resistor or the like is not Oh. The oscillating circuit of the present invention combines a capacitor and an inductor in parallel. [0054] Further, according to the above publication, the film thickness changes from the resistance component and the reactance component to the combined impedance, and the resultant impedance forms a straight line relationship with respect to the film thickness variation in a wide range, and the film thickness is obtained from the change relationship of the straight line. . However, in the present invention, 'the purpose is not to measure the film thickness in a wide range. The person who correctly predicts the end point of the polishing according to the change in the waveform of the feature before the end time of the grinding. 22 200912252 [0055] Further, the change in the waveform of the feature before the polishing end time is not a slight straight line change. According to the effect of the skin effect, there is a sharp change point. The person who correctly predicts the polishing end time point based on the feature points such as the change point and the sharp change rate before and after. [0056] Further, in accordance with the above publication, in paragraph 0027, the change in the amount of resistance relative to the change in the thickness of the conductive film is not shown in the circle 7 (b) (Attachment 1). The relationship between the change in the resistance amount and the thickness variation is that the resistance component R changes as the thickness changes from thick to thin. That is, in the region (a) of the extremely thin film thickness, the output of the resistance component R changes linearly, and when it becomes the region (b) of a certain thickness, the change in the resistance component R saturates, and then the film thickness becomes thick. The area (c) +, the output of the resistance component R is lowered. Here, in the case of the copper film, the point (a) represents about 1 〇〇〇 λ, the point (b) represents 2000 A to 3000 A, and the point (c) represents 5 〇〇〇 A or more. [0057] However, the behavior of the resistance component such as the thickness of the conductive film becomes larger depending on the film thickness, and then becomes smaller, and the behavior of the circle is shown in the balance of the resistance component and the electric k into the f" The phase is different from each other, and the action is not completely different according to the invention according to the effect of the broadening effect. [0058] In the present invention, the process of "incorporating the magnetic field line from the magnetic field line into the conductive crucible" _The force line leaks as the film thickness decreases, and then, when the magnetic field lines penetrate to a certain extent, the so-called full current is reduced according to the film product of the film), based on the reduction of the series of effects, the sharp change point The system 23 200912252 is generated. The inflection point is not simply the one that affects the frequency. As shown in the example of changing the inductor distance and the inductor diameter shown later, even the same frequency 'is still due to the inductor The diameter or the distance between the inductor and the conductive film changes the directivity of the magnetic field, and the magnetic field changes greatly as the intrusion behavior in the conductive film. The film thickness at the time of polishing decreases with respect to an inductor diameter and an inductor distance. The process has an inflection point based on the skin effect, but in the case of, for example, an inductor size of 1/1000 and an inductor distance, there is a change based on the agglomeration effect in the process of reducing the film thickness during grinding. The case of the curved point. This is clearly indicated, not only the frequency at that time in the shape of the inductor or the distance, etc., the directivity change of the magnetic field, depending on the skin effect, the intrusive characteristic of the magnetic field on the conductive film changes, In the present invention, a process of changing the film thickness by polishing from a state in which the magnetic field does not enter the conductive film to a state in which the magnetic field is continuously invaded is formed. The point at which the conductive film is removed is accurately predicted by the change in state. [0060] Thus, the change in the resistance component according to the broad effect in the present invention is in phase relationship with the resistance component and the reactance component from the conventional technique. The change in the resistance component is completely different. [0061] And 'in accordance with Patent Document 3 (Patent No. 3902064), first, in the paragraph of the prior art 〇〇 1 2. In the detection method of the polishing end point of the conventional eddy current sensor, since the oscillating frequency 24 200912252 used by the eddy current sensor is about 7 Μ 1 较小, the conductivity of the object to be polished 骐In the case of a relatively large thickness, a large eddy current loss can be detected. However, when the conductive film is polished to make the film thickness extremely thin, the magnitude of the eddy current loss is small, and in this case, for example, about 1000 A or less. The film thickness detection system becomes difficult. That is, since the conventional current sensor has a low frequency of vibration, it is detected on the polishing end point of the polishing apparatus which requires the film thickness detection accuracy of the angstrom level. There is a problem that the accuracy is insufficient. [0622] It is also revealed that a thick film thickness or a thin film thickness can also infiltrate a magnetic field into a film, and simply monitor the film according to the magnitude of the current caused by the magnetic field. Thick method. [0063] However, in the present invention, when the conductive film is thick, the thickness of the conductive film is not considered to be a problem. The magnetic field does not intrude into the conductive (4) due to the effect of the broadening, and therefore is not required. A large full current is detected. In addition, in the case where the film thickness is gradually reduced to the extent of the deletion, even the non-directional magnetic field 'because the through-partial conductivity 形成 becomes full with the decrease of the material: the flow generates a repulsive magnetic field, so the accuracy can be Good land check out. It is not intended to measure the film thickness even with a thick film thickness, because the behavior of the (4) in the vicinity of the sexually-removed position is well predicted. The vibration frequency of [0064] is grasped as the frequency: the time gradient of the full-current sensor and the time gradient of the frequency and the calculation of the oscillation frequency 'money, and the determination of the grinding end point according to the characteristic point . Fig. 25 200912252 5 ( a) shows the trajectory of the time t of the oscillating disk frequency from the time of the cat, and the circle 5 (b) shows the trajectory of the differential value (Attachment. [ 0065] The action system of this vibration frequency The behavior of the vibration frequency monotonously decreasing is shown. The judge X of the polishing end point is performed at the lowest point of the monotonic reduction point of the vibration frequency, and the change point in the reduction of the green adjustment is found by the differential waveform to determine the end point. ^ [0066] However, in the context of the present invention, such a vibration frequency is different. That is, in the present invention, the process of reducing the film thickness by grinding, the vibration frequency is based on the skin effect of the conductive film. And as the film thickness decreases, it temporarily rises, then falls again, and has a peak near the end point. This behavior is caused by the process of making the magnetic field from invading to invading the conductive film according to the skin effect. The behavior shown in the prior art example is significantly different. [0067] Moreover, the present invention detects the portion of the inflection point that rises and falls and the feature near the inflection point, and predicts the end time of the polishing with high precision. Point. Further, in Patent Document 3, the spiral-shaped sensor coil is disposed to be orthogonal to the substrate, but in contrast, in the coil of the present invention, a planar inductor is disposed in parallel with the substrate. In the configuration of the device, it is also significantly different. [0069] Further, as shown in the paragraph 〇〇32, in the patent document 3, it is shown that the resistance component increases once and decreases with the decrease of the film thickness. However, 26 200912252 is a behavior that appears to be non-integrated. In the circuit shown in the picture, the inflection point caused by the balance of the resistance component and the reactance component in the phase difference is also known as ' The inflection point in the present invention is completely different from such an inflection point. As described earlier, the 'inflection point varies greatly depending on the size, shape, or distance of the conductive film to the coil, depending on the setting. There is also a case where the behavior according to the skin effect is not seen even in the high frequency band. [0070] In the present invention, the conductivity, the magnetic permeability and the frequency, the shape of the inductor, and the shape of the conductive film are appropriately set. Electricity The distance between the sensor and the conductive film, etc., in the process of reducing the film thickness by polishing, the state in which the oscillation frequency has an inflection point according to the skin effect, and the end of the polishing is accurately predicted according to the characteristics of the waveform. [Invention Effect] [0071] The conductive film on the circle monitors the domain that changes according to the f/ϊ effect of the conductive film to make the inductor close to the crystal
申請專利範圍第1項記載的發明 〔 0072〕Patent Application No. 1 [0072]
研磨除去量的不均、 、平均骐厚、研磨 I:的不均、殘餘骐 27 200912252 厚的不均、殘制的形狀等任意之資料使研磨精度提升。 〔 0073〕 中請專利範S1帛3項記載的發明,係透過在晶圓面内 的多個部位’同時地檢出共振頻率的波形,可由共振頻率 的波形之時間的偏差,即時檢知或預測研磨均一性。 〔 0074〕 申請專利範圍第4項記載的發明,係透過使用二次元 平面電感器,讓磁場難以進入導電性膜内,集膚效應的影 響變得顯著,可精度佳地估計膜厚不均或殘餘膜厚等。 〔 0075〕 申請專利範圍第5項記載的發明,由於依伴隨膜厚減 少而産生的渦電流所誘起之集膚效應會引起特徵的變化, 所以能透過監視經過其特徵的變化之部分的時間而即時地 精度佳地求取研磨量。 〔 0076〕 申請專利範圍第6項記載的發明,係於晶圓面内的複 數個位置’監視經過磁力線之特徵的變化之部分的時間, 再由其經過時間之不均來求取研磨量,藉此可更高速地求 取研磨量。 〔 0077〕 申請專利範圍第7項記載的發明,係由經過被引起於 導電性膜之特徵的磁力線變化的部分時之經過時間,求取 研磨除去量的不均或在複數個位置之各個膜厚量,藉此可 精度佳地監視研磨量。 〔 0078〕 28 200912252 在上述之本發明中,由於會顯現含有依據特有的集膚 效應之變曲點之特徵的磁力線變化,所以如同申請專利範 圍第8項所記載的發明,可由渦電流、互感、阻抗變化、 共振頻率變化等當中的一種或複數種資料高精度地預測研 磨量。 〔本發明最佳實施形態〕 〔 0079〕 本發明係利用以下研磨結束時間點之預測方法使強的 磁力線不會及於導電性膜内所形成之微細配線,其結果係 抑制依電磁誘導所引起之渦電流的發生,將渦電流引發的 焦耳熱損抑制成極小,而無關乎因初期骐厚之偏差或間陈 的變化等所造成之電氣條件的變動’達成所謂精度佳地預 測/檢出研磨結束時間點之目的。該方法之特徵為:在一邊 供給研磨漿或藥液、一邊使研磨墊等之加工工具與具有導 電性膜的晶圓滑動以進行導電性膜的除去加工的研磨工程 中,使電感器接近晶圓上的導電性膜,監視被該電感器所 形成的磁力線引起於晶圓的導電性膜上、並依以導電性骐 的材質為一因子的集膚效應而變化的磁力線,一邊進行晶 圓面的研磨加工、一邊即時地估計研磨量。 C實施例1〕 〔 0080〕 囫1顯不化學機械研磨裝置1,圓盤形的平臺2係被 安裝於利用了馬達3的驅動機構4之上,平臺2的上面貼 附有研磨墊5 ^配置在平臺2的上方且從平臺2旋轉中心 變位的位置之研磨頭6’係比平臺2還小徑的圓盤形,其 29 200912252 下面安跋有屬研磨對象的晶圓在研磨工程中,從藥液 供給裝置(未圊示)將研磨藥液或研磨漿滴到研磨墊5的 上面’研磨頭6被下降到晶圓W朝研磨墊5上面接觸的高 度’且平臺2和研磨頭6係被分別旋轉驅動以研磨晶圓w 之被研磨面(下面)。在研磨墊5之下的平臺2表面埋入有 平面狀的電感器型感測器34,平臺2每一旋轉,電感器型 感測器34係通過被裝設在研磨頭6之晶圓w的下面。 〔0081〕 囷2係顯示研磨結束時間點的預測/檢出裝置33之構 成例的圓’圓2(a)為方塊圖,圊2(b)為平面狀電感器 之其他構成例的圖,圊2(c)為圓2(b)之平面狀電感器 的剖面圖。構成研磨結束時間點的預測/檢出裝置33中之 高頻電感器型感測器34的主體之振盪電路35為,在成為 電感L的二次元的平面狀電感器36,串聯連接作為電容c〇 的集中常數電容器37而構成LC電路》平面狀電感器36係 在由絶緣物所成的方形等的基板36a上,使用Cu等的導電 物質而建構成婉纟延(meander)形。 〔 0082〕 平面狀電感器36除了圊2(a)所示螺旋形以外,如 同圖2(b)所示之平面狀電感器41般,在方形的基板4 la 上建構成婉蜒形亦可。又,亦可作為圓形的螺旋。二次元 的平面狀電感器36、41係在由玻璃環氧或紙酚等之絶緣物 所成的基板36a、41a上成膜了 Cu等的導電膜之後,利用 触刻等方式製作,可將線寬製作成非常地微細化,整體形 狀亦如圖2 ( c)所示’可小型化成一邊是23mm程度的方 30 200912252 形等。且透過平面狀電感器36、41之小型化可有效地產生 微小磁場,可在磁場未深深地浸透於導電性骐28内部之 下,精度佳地檢出在導電性膜28被除去的終點附近之變化 舉動》 〔 0083〕 來自振盪電路35的輸出信號被輸入到由運算放大器 等所構成之放大器38,放大器38的輸出被輸入到由電阻 等所構成之回授網路39。回授網路39的輸出信號被正回 授於平面狀電感器36,藉此構成含有該平面狀電感器36 的振盪電路35。 〔 0084〕 振盈電路35,基本上乃如圖3之構成例所示,其振盘 頻帶f係如(數式1 )所示,形成由平面電感器36的電感 L和集中常數電容器37的電容C0所決定的柯匹次型之振 盪電路》 〔 0085〕 〔數式1〕Unevenness of polishing removal, average thickness, unevenness of polishing I: residual 骐 27 200912252 Any data such as thick unevenness and residual shape improves polishing accuracy. [0733] In the invention described in the patent document S1帛3, the waveform of the resonance frequency is detected simultaneously at a plurality of locations in the wafer surface, and the time difference of the waveform of the resonance frequency can be immediately detected or The grinding uniformity is predicted. [0074] According to the invention of claim 4, the use of the secondary element planar inductor makes it difficult for the magnetic field to enter the conductive film, and the effect of the skin effect becomes remarkable, and the film thickness unevenness can be accurately estimated. Residual film thickness and the like. [0075] According to the invention of claim 5, since the skin effect caused by the eddy current caused by the decrease in the film thickness causes a change in characteristics, it is possible to monitor the time passing through the change of the characteristic. The amount of grinding is accurately determined in real time. [0076] The invention according to claim 6 is characterized in that the plurality of positions in the wafer surface are monitored for the time when the change in the characteristics of the magnetic lines of force is monitored, and the amount of polishing is determined by the unevenness of the elapsed time. Thereby, the amount of grinding can be obtained at a higher speed. [0077] The invention according to the seventh aspect of the invention is the method of obtaining the unevenness of the amount of polishing removal or the film at a plurality of positions by the elapsed time when the portion of the magnetic field line which is characteristic of the conductive film is changed. The thickness is used to monitor the amount of grinding with high precision. [0078] 28 200912252 In the above-described invention, since the magnetic line change including the characteristic of the inflection point according to the specific skin effect is exhibited, the invention described in claim 8 can be eddy current, mutual inductance. One or a plurality of kinds of data such as impedance change, resonance frequency change, etc., predict the amount of grinding with high precision. BEST MODE FOR CARRYING OUT THE INVENTION [0079] The present invention utilizes the following method for predicting the end of polishing time to make strong magnetic lines of force less than the fine wiring formed in the conductive film, and as a result, suppresses electromagnetic induction. The occurrence of the eddy current suppresses the Joule heat loss caused by the eddy current to a minimum, irrespective of variations in electrical conditions caused by variations in initial thickness or variations, etc. The purpose of grinding the end time point. This method is characterized in that the inductor is brought close to the crystal in a polishing process in which a polishing tool or a chemical solution is supplied while a processing tool such as a polishing pad is slid with a wafer having a conductive film to remove a conductive film. The conductive film on the circle monitors the magnetic field lines formed by the inductor and causes the magnetic field lines on the conductive film of the wafer to change depending on the skin effect of the conductive material. The surface is ground and the amount of polishing is estimated instantaneously. C. Example 1] [0080] The 化学1 display chemical mechanical polishing apparatus 1 is mounted on a disk-shaped stage 2 on a drive mechanism 4 using a motor 3, and a polishing pad 5 is attached to the upper surface of the stage 2 ^ The polishing head 6' disposed above the platform 2 and displaced from the center of rotation of the platform 2 is a disc shape having a smaller diameter than the platform 2, and 29 200912252 is mounted with a wafer to be polished in the grinding process. The abrasive liquid or slurry is dropped from the liquid supply device (not shown) onto the upper surface of the polishing pad 5 'the polishing head 6 is lowered to the height of the wafer W contacting the polishing pad 5' and the stage 2 and the polishing head The 6 series are rotationally driven to polish the polished surface (bottom) of the wafer w. A planar inductor-type sensor 34 is embedded in the surface of the stage 2 below the polishing pad 5. Each of the stages 2 is rotated, and the inductor-type sensor 34 is passed through a wafer mounted on the polishing head 6. Below.囷2 is a block diagram showing a circle 'circle 2 (a) of a configuration example of the prediction/detection device 33 at the polishing end time point, and 圊 2 (b) is a view showing another configuration example of the planar inductor.圊2(c) is a cross-sectional view of a planar inductor of circle 2(b). The oscillation circuit 35 of the main body of the high-frequency inductor type sensor 34 in the prediction/detection device 33 constituting the polishing end time point is a planar inductor 36 which is a quadratic element of the inductance L, and is connected in series as a capacitor c. The lumped constant current capacitor 37 constitutes an LC circuit. The planar inductor 36 is formed on a substrate 36a made of an insulator or the like, and is formed into a meander shape by using a conductive material such as Cu. [0082] The planar inductor 36 has a spiral shape as shown in FIG. 2(a), and like the planar inductor 41 shown in FIG. 2(b), the dome substrate 4a may be formed in a square shape. . Also, it can be used as a circular spiral. The planar inductors 36 and 41 of the secondary element are formed by forming a conductive film of Cu or the like on the substrates 36a and 41a made of an insulating material such as glass epoxy or paper phenol, and then forming them by means of etching or the like. The line width is made to be extremely fine, and the overall shape is also as shown in Fig. 2 (c), which can be miniaturized into a square 30 200912252 with a side of 23 mm. Further, by miniaturizing the planar inductors 36 and 41, a minute magnetic field can be efficiently generated, and the magnetic field is not deeply penetrated inside the conductive crucible 28, and the end point at which the conductive film 28 is removed can be accurately detected. In the vicinity of the change behavior [0083] The output signal from the oscillation circuit 35 is input to an amplifier 38 composed of an operational amplifier or the like, and the output of the amplifier 38 is input to a feedback network 39 composed of a resistor or the like. The output signal of the feedback network 39 is positively fed back to the planar inductor 36, thereby constituting the oscillation circuit 35 including the planar inductor 36. [0084] The oscillation circuit 35 is basically shown in the configuration example of FIG. 3, and the vibration plate frequency f is as shown in (Expression 1), and the inductance L of the planar inductor 36 and the lumped constant capacitor 37 are formed. The oscillation circuit of the Kepi type determined by the capacitor C0" [0085] [Expression 1]
〔 0086〕 前述放大器38的輸出端子連接計頻器4〇。從該計頻 器40將表示後述的骐厚基準點之檢出信號等以數位方式 朝外部輸出。藉由將檢出信號輸出以數位方式作傳送,防 止雜訊之影響及輸出衰減。又,可獲得膜厚資料之管理容 易性。 31 〔 0087〕 200912252 透過將高頻電感器型感測器34的振盪電路35與監視 其振盘(共振)頻率變化用的計頻器4〇接近地作配置,在 該振盪電路35與計頻器40間之配線/接線部分形成分布常 數電路以防止電感或電容不必要地變大,成為可精度佳地 檢出被帶來高頻電感器型感測器34附近之伴隨導電性骐 28研磨的進行之磁力線的變化。 〔 0088〕 研磨結束時間點的預測/檢出裝置33係平面狀電感器 36除外的其他構成零件乃至電路被丨c (積體電路)化並内 裝在封裝33a。前述平面狀電感器36被薄的絶緣膜被覆並 固定於封裝33a的表面。當被封裝化之研磨結束時間點的 預測/檢出裝置33被組裝到前述化學機械研磨裝置!時,如 圊1所示般,平面狀電感器36係被組裝成與晶圓w的表面 部之導電性膜對峙。 〔 0089〕 又’構成振盪電路35的集中常數電容器37係電容成 為可變’高頻電感器型感測器34係成為在振盪頻帶之範圍 内可選擇振盪頻率。 〔 0090〕 本實施例中係依據研磨中的導電性膜28已成為對應 既定的表皮深度δ之膜厚的情況之磁力線變化而進行後述 之膜厚基準點的檢出。導電性膜28中之既定的表皮深度δ 係依存於導電性膜28的材質與高頻電感器型感測器34的 振盡頻率ί而決定成如(數式2)。 〔0091〕 32 (2) 200912252 〔數式2〕 δ yj mm .. 〔0092〕ω=2πί、 〔 0093〕 β為透磁率 、σ為導電率。 叩且 :…度δ可比既定的導電性膜28的初期膜 厚還小’成為比研磨終期既研磨了除埋人部以外的部分之 ^電性膜28 _厚紅的方式選擇高頻電❹型感測器 的振錢杯在研磨除去對象之導電性膜28的材質是 Cu的情況,振盪頻帶選擇20MHz以上。 〔 0094〕 在此,針對前述之「對應表皮深度的膜厚」及「依集 廣效應而產生之磁力線變化」,使用圖4的(a)〜⑷作 說明》圊4係顯示電磁模擬了由線圈所產生的磁場是導體 膜上配列成什麼樣朝向(圖4(a)〜⑷各圓中下方的 箭頭-)之結果的圖。此乃顯示在線圏流 最大的情況…⑷係來自感測器的振嶋是: 且導體膜膜厚為0.2" m的情況’圖4 (b)係來自感測器 的振虚頻率是1MHz且導體膜膜厚為1//m的情況,圖4(c) 係來自感測器的振盪頻率是侧ίζ且導趙膜膜厚為〇, 2心 的情況,圖4 (d)係來自感測器的振盪頻率是4〇ΜΗζ且導 雜膜膜厚為丨Vin的情況。 〔 0095〕 電磁模擬之設定為,形成磁場用的電感器係設為未具 指向性的平面狀電感器。前述Γ對應表皮深度的膜厚」係 指,r依集廣效應而產生磁力線變化之膜厚」^以感測器的 33 200912252 振堡頻率是1MHz而言,存在於線圈下側的導趙膜上之磁力 線係朝向縱方向。以此頻率而言,即便膜厚& 1//〇]及〇 2 vm’磁力線還是貫通導體膜内(圊4(a)、囷在 磁力線貫通這樣的導體膜内之情況,如同在習知例所示,在 導體膜内部發生的渦電流係伴隨著膜厚減少而減少。因 而,在1MHz的情況,以以下的膜厚而言’因為是單 調的舉動’所以集廣效應未出現,認為「對應表皮深度的 膑厚」也至少是比l#m還厚的膜厚。 〔 0096〕 相對地,以感測器的振盪頻率是40MHz而言,在導體 表面之磁力線朝向很明顯是水平,以膜厚是1 β m而言,幾 乎不會進入導體内部(圖4 (d))e與先前振盪頻率是1MHz 且膜厚為1/zm的情況(圖4 (b))比較之下,可知進入於 導體膜的磁力線之朝向是不同的。 〔 0097〕 但是,當振盪頻率是40MHz且導體膜薄到(圏 4 ( c )),僅一部份磁力線是朝向導體膜内部方向。此乃示 出即使導體膜是Cu ’當成為某薄度時,一部份磁力線是會 貫通導體膜内的。 〔 0098〕 在此40 MHz的交替變化之磁力線的情況,對應於集廣 效應’導趙膜内的磁力線之貫通狀態會變化。因貫通磁力 線徐除增加的影響,約在700 Α前後頻率急劇上昇β此外, 以膜厚是1/zm以上而言’磁力線幾乎不貫通。因而,在此 情況’當設為磁力線貫通或不貫通的境界之犋厚時,「對應 34 200912252 表皮冰度的骐厚」可以是約1 // m左右。由此亦可知,當振 盈頻率設高為40MHz,使用平面狀電感器時,磁力線幾乎 不進入lvm厚度的Cu導體膜内,此乃係依據集廣效應者。 〔 0099〕 在是Cu導體膜且振盪頻率為40MHz的情況,當設cu 的導電率為58xl〇6S/m時,表皮深度δ成為9. 3//m。在計 算上’當膜厚是1 V m,磁力線就足以進入導體膜内,但是 由於使用平面狀電感器,磁力線未具指向性,所以實際上 在振盪頻率是40ΜΠζ的情況,即使膜厚為lym,磁場還是 會因為集膚效應而不侵入於導體膜内。隨著導體膜變薄, 一部份磁力線進入導體膜内,產生少許渦電流。並非由此 而積極地利用渦電流來進行膜厚測定者,而是利用在成為 終點附近之薄的膜厚時依集膚效應而稍漏洩/貫通的磁力 線,利用引起於導體膜内之互感的變曲點(極大點)可監 視該導體膜之終點附近的膜厚狀態。 〔0100〕 此互感亦對應於一次側線圈的阻抗成份。在求取 線圈電路系之阻抗變化時’求取引起於導體膜的渦電流變 化與線圈側阻抗變化之關係。在形成如圖5所示的等價電 路,直設定了各個構成要素之情況,電路方程式係以數式 3來表示。 [0101〕 〔數式3〕 35 200912252 f ί ^·2Νί//.—¥Μ Μ + + ¢//.1¾^^ II 12 (3)-(4 〔0102〕 在此,il、i2分別為在一次側與二次側流通的電流, 於一次側,設定v的電壓施加於線圈,在具有一定的各振動 頻率之交流ω的情況,分別表示為 〔0103〕 〔數式4〕 /丨=Re(/〆) /2=Re(/2^) v = KQ(Vej0)l) 〔0104〕 而(數式3)和(數式4 )係表示如次。 〔0105〕 〔數式5〕[0086] The output terminal of the aforementioned amplifier 38 is connected to the counter 4〇. From the counter 40, a detection signal indicating a thickness reference point, which will be described later, and the like are output to the outside in a digital manner. By transmitting the detected signal digitally, the effects of noise and output attenuation are prevented. Further, the management ease of the film thickness data can be obtained. 31 [0087] 200912252 By arranging the oscillation circuit 35 of the high-frequency inductor type sensor 34 and the counter 4〇 for monitoring the frequency of the vibration (resonance) of the high-frequency inductor type sensor 34, the oscillation circuit 35 and the frequency measurement are performed. The wiring/wiring portion between the devices 40 forms a distributed constant circuit to prevent the inductance or the capacitance from becoming unnecessarily large, so that the accompanying conductivity near the high-frequency inductor type sensor 34 can be accurately detected. The change of the magnetic field line. [0088] The prediction/detection device 33 at the polishing completion time point is a component other than the planar inductor 36, and the circuit is c (integrated circuit) and is housed in the package 33a. The planar inductor 36 is covered with a thin insulating film and fixed to the surface of the package 33a. When the prediction/detection device 33 at the end of the polishing end of the encapsulation is assembled to the aforementioned chemical mechanical polishing device!, as shown in FIG. 1, the planar inductor 36 is assembled to be the surface portion of the wafer w. The conductive film is opposite to the crucible. [0089] Further, the lumped constant capacitor 37 constituting the oscillation circuit 35 has a variable capacitance. The high frequency inductor type sensor 34 has an oscillation frequency selectable within the range of the oscillation frequency band. [0090] In the present embodiment, the film thickness reference point to be described later is detected in accordance with the change in the magnetic field line in the case where the conductive film 28 during polishing has a film thickness corresponding to a predetermined skin depth δ. The predetermined skin depth δ in the conductive film 28 is determined by the material of the conductive film 28 and the vibration frequency ί of the high-frequency inductor type sensor 34 (Expression 2). [0091] 32 (2) 200912252 [Expression 2] δ yj mm .. [0092] ω = 2πί, [0093] β is the permeability and σ is the conductivity. Further, the degree δ can be made smaller than the initial film thickness of the predetermined conductive film 28, and the high-frequency electric enthalpy is selected in such a manner that the electric film 28 _ thick red is polished at the end of the polishing process except for the portion other than the buried portion. In the case where the material of the conductive film 28 to be polished and removed is Cu, the vibration cup of the type sensor is selected to have an oscillation frequency band of 20 MHz or more. [0094] Here, the "film thickness corresponding to the depth of the skin" and the "change in the magnetic field line generated by the broadening effect" are described using (a) to (4) of Fig. 4, and the 圊4 system shows the electromagnetic simulation. The magnetic field generated by the coil is a result of what kind of orientation is arranged on the conductor film (the arrow - below the respective circles in FIGS. 4(a) to (4)). This is the case where the maximum turbulence is displayed... (4) The vibration from the sensor is: and the film thickness of the conductor film is 0.2 " m'. Figure 4 (b) The vibration frequency from the sensor is 1 MHz. When the film thickness of the conductor film is 1/m, Figure 4(c) shows that the oscillation frequency from the sensor is side and the film thickness is 〇, 2, and Figure 4 (d) is from The oscillation frequency of the sensor is 4 〇ΜΗζ and the film thickness of the conductive film is 丨Vin. [0095] The electromagnetic simulation is set such that the inductor for forming a magnetic field is a planar inductor having no directivity. The film thickness corresponding to the skin depth of the Γ refers to the film thickness of the magnetic field change caused by the r-wide effect of the sensor. 33. The sensor is 33. The 200912252 vibration frequency is 1 MHz, and the film is present on the lower side of the coil. The magnetic lines of force are oriented in the longitudinal direction. At this frequency, even if the film thickness & 1//〇] and 〇2 vm' magnetic field lines pass through the conductor film (圊4(a), 囷 is in the conductor film through which the magnetic flux penetrates, as in the conventional In the example, the eddy current generated in the inside of the conductor film is reduced with the decrease in the film thickness. Therefore, in the case of 1 MHz, the effect of the broadening effect does not appear because of the following film thickness. "The thickness of the corresponding skin depth" is at least a film thickness thicker than l#m. [0096] In contrast, the magnetic field line on the surface of the conductor is obviously horizontal when the oscillation frequency of the sensor is 40 MHz. In the case where the film thickness is 1 β m, it hardly enters the inside of the conductor (Fig. 4 (d)). e is compared with the case where the previous oscillation frequency is 1 MHz and the film thickness is 1/zm (Fig. 4 (b)). It can be seen that the direction of the magnetic lines of force entering the conductor film is different. [0097] However, when the oscillation frequency is 40 MHz and the conductor film is as thin as (圏4 (c)), only a part of the magnetic lines of force are directed toward the inside of the conductor film. It shows that even if the conductor film is Cu', when it becomes a certain thinness, a part of the magnetic force It will penetrate through the conductor film. [0098] In the case of the alternating magnetic field line of 40 MHz, the penetration state of the magnetic field line in the film is changed corresponding to the effect of the broadening effect. In the case where the film thickness is 1/zm or more, the magnetic field lines are hardly penetrated. Therefore, in this case, when the magnetic field is penetrated or not penetrated, the corresponding 34 200912252 The thickness of the skin ice can be about 1 / m. It can be seen that when the vibration frequency is set to 40MHz, when the planar inductor is used, the magnetic field lines hardly enter the Cu conductor film with the thickness of lvm. 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 In the calculation, when the film thickness is 1 V m, the magnetic field lines are enough to enter the conductor film, but since the magnetic field lines are not directional due to the use of the planar inductor, the actual oscillation frequency is 40 ,, even if the film thickness is Lym The magnetic field does not intrude into the conductor film due to the skin effect. As the conductor film becomes thinner, a part of the magnetic lines of force enter the conductor film, causing a little eddy current. Therefore, the eddy current is not actively used to determine the film thickness. However, the magnetic flux which is slightly leaked/penetrated by the skin effect at the thin film thickness near the end point is used, and the end point of the conductor film can be monitored by the inflection point (maximum point) of the mutual inductance in the conductor film. The film thickness state is nearby. [0100] This mutual inductance also corresponds to the impedance component of the primary side coil. When the impedance change of the coil circuit system is obtained, the relationship between the eddy current change caused by the conductor film and the coil side impedance change is obtained. In the case where an equivalent circuit as shown in Fig. 5 is formed, each component is directly set, and the circuit equation is expressed by Equation 3. [0101] [Expression 3] 35 200912252 f ί ^·2Νί//.—¥Μ Μ + + ¢//.13⁄4^^ II 12 (3)-(4 [0102] Here, il and i2 are respectively The current flowing through the primary side and the secondary side is applied to the coil on the primary side, and the alternating voltage ω having a certain vibration frequency is expressed as [0103] [Expression 4] / 丨 = Re(/〆) /2=Re(/2^) v = KQ(Vej0)l) [0104] and (Expression 3) and (Expression 4) are expressed as follows. [0105] [Expression 5]
Rx + jmL joM X ―-^ V jcoM R2 + jaL2 A 0 ·· · 〔0106〕 此數式的解係如次式。 〔0107〕 〔數式6〕 J __尺2 + J·①L2__ 36 200912252 (/?, + j〇)Lx )(R2 + j〇)L2) + co2M2 ^ 〔0108〕 由線圈側所見之阻抗係成為以下那樣。 〔數式Ή R2+ jc〇L2 τ + ιω L ^_^2ω2Μ2 Z = — = i?, + jmLx + —Rx + jmL joM X ―-^ V jcoM R2 + jaL2 A 0 ·· · [0106] The solution of this number is as follows. [0107] [Expression 6] J __ 尺 2 + J·1L2__ 36 200912252 (/?, + j〇) Lx ) (R2 + j〇) L2) + co2M2 ^ [0108] The impedance system seen from the coil side It becomes the following. [Expression Ή R2+ jc〇L2 τ + ιω L ^_^2ω2Μ2 Z = — = i?, + jmLx + —
/. /?. 4- irnT/. /?. 4- irnT
〔0109〕[0109]
系的阻抗實部之變化。 〔0110〕 圖6係顯示針對使用了平面電感器的情況之阻抗實部 的膜厚相依性,利用2次元電磁模擬所獲得之結果。以4〇MH z的情況而言’在G.lp以下具有變曲點,之後阻抗急劇 減少。相肖地’在1MHz的情況,·3J*知係與膜厚相依而單 調地減少。由此可知,像本題那樣的變曲點,首先是依處 理的頻率之大小而顯現的。又,這樣的變曲點之出現,從 基於磁力線之朝向的變化可理解係由圖4所示那樣的集廣 效應之影響所致。 〔0111〕 37 200912252 但是’只要頻率設為40MHz而電感器形狀作成平面電 感器的話’則是否依集膚效應的影響而顯現變曲點就不一 定。作為其事例,係在使平面電感器充分接近導電性膜的 情況,與圖4同樣地透過2次元有限要素的模擬作了確認。 〔0112〕 在此’使平面電感器比先前所示距離還接近1/1〇〇〇 而設為2.4//1Π,線圈的大小也作1/1〇〇〇的半徑n ^^計 算。在線圈的頻率設為4〇MHz,導體膜設為Cu而膜厚設為 1 A m並經計算後,即使是1 β m的膜厚,還是與圊4的情 况不同’會有多的磁力線貫通。但是’當頻率提升到1 Ghz 時,磁力線幾乎變得不貫通(圖示省略 〔0113〕 圓7顯示在線圈徑為1/1〇〇〇、線圏和導電性膜距離 為1/ 1000的情況中,線圈側阻抗的實部變化。可知即使 疋40MHz的頻率還是未具有變曲點。當頻率提升到1 ghz 時,在1 // m附近產生變曲點》此乃先前進入導體内的磁場 之朝向,可知道因為集廣效應的影響而產生了變曲點。 〔0114〕 ’ 由以上的實驗結果可知,在受到集廣效應的影響而要 形成變曲點時,不是單單將頻率設高並使用平面電感器就 可以的》適當地保有線圈和導電性膜之距離或是線圈的大 小等亦變重要。又,研磨對象膜的導電率及透磁率等,其 材料的物性之起因,由將鎢作同樣研磨的情況之波形就可 清楚。 〔0115〕 38 200912252 因而’為了利用所謂磁力線依集廣效應而侵入/不侵入 導電性骐内的舉動,係可透過適當地選擇頻率、電感器的 形狀或大小、電感器與導電性膜之距離、導電性膜的導電 率、透磁率而達成。係找出設定成依如此集膚效應之影響 的變曲點可顯現於研磨終點附近,設定檢出其變曲點的計 算邏輯而精度佳地預測研磨結束點的新方法,並作為本發 明之要旨者。 〔0116〕 其次’兹針對研磨結束時間點預測方法之實際的運用 作敘述。圖8係顯示平臺上的電感器對晶圓之轨跡’晶圓 的A點至_ E &中之共振頻率波形的一關係例顯示於圊9。 在此,係不出共振頻率之峰值的出現在c點最早,B點和〇 點接於其後,A點和£點變最慢,屬晶圓中心部的。點之 研磨率最快,而外周部之A點和E點慢。圖1〇顯示圖9中 的時間點1和時間點2之Λ點至E點中的研磨量》從連結 各點的曲線形狀可知晶圓的研磨形狀(殘膜形狀 〔0117〕 圖11示出利用本發明之研磨結束時間點的預測方法 在進行研Cu膜時之參考波形,在臈厚710Α具有共振頻率 的峰值。如同圖中所示,若事先對參考波形之各位置求取 對應的膜厚’由實際得到的波形之變化率可知到在各位置 中之殘餘膜厚。 〔0118〕 而且,由在既定的時間於各位置之膜厚的不均,即時 地求取殘膜之不均一性》其中在以下的式子中,f丨是在位 39 200912252 置i的骐厚。 〔0119〕 〔數式8〕The change in the real part of the impedance of the system. [0110] Fig. 6 shows the results obtained by the 2-dimensional electromagnetic simulation for the film thickness dependence of the real part of the impedance in the case where the planar inductor is used. In the case of 4 〇 MH z, there is an inflection point below G.lp, and then the impedance is drastically reduced. In the case of 1 MHz, the 3J* knowledge system is monotonously reduced depending on the film thickness. From this, it can be seen that the point of variation such as this one is first manifested by the frequency of the processing. Further, the occurrence of such a change point is understood to be caused by the influence of the widening effect as shown in Fig. 4 from the change in the direction of the magnetic line. [0111] 37 200912252 However, if the frequency is set to 40 MHz and the inductor shape is a planar sensor, it is not necessary to show the inflection point depending on the effect of the skin effect. As an example of this, in the case where the planar inductor is sufficiently close to the conductive film, it is confirmed by simulation of the quaternary finite element as in Fig. 4 . [0112] Here, the planar inductor is made closer to 1/1 比 than the previously shown distance and is set to 2.4//1 Π, and the size of the coil is also calculated as the radius n ^^ of 1/1 。. When the frequency of the coil is 4 〇 MHz, the conductor film is Cu and the film thickness is 1 A m, and even after the calculation, the film thickness of 1 β m is different from that of 圊4. Through. However, when the frequency is raised to 1 Ghz, the magnetic lines of force become almost opaque (the illustration is omitted [0113]. The circle 7 shows the case where the coil diameter is 1/1 〇〇〇, the coil turns and the conductive film distance is 1/1000. In the middle, the real part of the coil side impedance changes. It is known that even the frequency of 疋40MHz does not have an inflection point. When the frequency is raised to 1 ghz, an inflection point is generated around 1 // m. This is the magnetic field previously entering the conductor. In the orientation, it can be known that the inflection point is generated due to the effect of the collective effect. [0114] ' From the above experimental results, it is known that when the inflection point is formed due to the effect of the broadening effect, the frequency is not set high alone. It is also possible to properly maintain the distance between the coil and the conductive film or the size of the coil by using a planar inductor. Moreover, the conductivity and permeability of the film to be polished, etc., are caused by the physical properties of the material. The waveform of the case where the tungsten is polished in the same manner is clear. [0115] 38 200912252 Therefore, in order to utilize the so-called magnetic lines to intrude/not intrude into the conductive crucible according to the broadening effect, it is possible to appropriately select The frequency, the shape or size of the inductor, the distance between the inductor and the conductive film, the conductivity of the conductive film, and the magnetic permeability. It is found that the inflection point set to be affected by such a skin effect can be seen in the grinding. In the vicinity of the end point, a new method of predicting the calculation point of the inflection point and accurately predicting the end point of the polishing is set as the gist of the present invention. [0116] Secondly, the actual application of the method for predicting the end time of polishing is performed. Figure 8 shows an example of the relationship between the inductor-to-wafer track on the platform, the resonant frequency waveform in the A-to-_E & wafer. The resonance is not shown here. The peak of the frequency appears at the earliest point c, the B point and the 〇 point are followed, and the A point and the point become the slowest, belonging to the center of the wafer. The grinding rate of the point is the fastest, and the point A of the outer circumference is E point is slow. Fig. 1 shows the amount of polishing from time point 1 and time point 2 in Fig. 9 to point E. The shape of the wafer is known from the shape of the curve connecting the points (residual film shape [0117] Figure 11 shows the predicted side of the grinding end time point using the present invention. The reference waveform of the method for conducting the Cu film has a peak of the resonance frequency at a thickness of 710 。. As shown in the figure, if the corresponding film thickness is obtained for each position of the reference waveform in advance, the rate of change of the waveform actually obtained is obtained. The residual film thickness at each position is known. [0118] Further, the unevenness of the residual film is obtained instantaneously from the unevenness of the film thickness at each position for a predetermined period of time, wherein in the following formula, f丨 is the thickness of the position at 2009 3912252. [0119] [Expression 8]
〔0120〕[0120]
的情況,不岣一性(Nonunif) 〔0121〕 〔數式9〕The situation is not uniform (Nonunif) [0121] [Expression 9]
Nonunif = 〇〇(%) 〔0122〕 又,在其他方法方面,亦可由初期膜厚減去殘餘骐厚 而求得除去膜厚,再依除去膜厚的不均來求取不均一性。 〔0123〕 ° 抑或’從已到達既定的變化率(既定的研磨量)的時間 來求取研磨量之不均一性亦可。 〔0124〕 〔數式10〕 £ / :在位置/的除去膜厚 (·(:在位置/達到X的硏磨量之時間 在既定之變化率位置的既定硏磨量 40 〔0125〕 200912252 而且,從(數式8)和(數式9)可求取研磨量之不均 一性0 〔0126〕 此外,在圖1中係顯示在平臺2之上面配置著一個電 感器型感測器34之例子,但如圊丨2所示,在平臺2的上 面將複數個電感器型感測器34朝半徑方向排列配置,在平 臺2上貼研磨墊(未圖示),同時地監視於晶圓的各位置之 共振頻率的波形亦可。此情況為’從複數個電感器型感測器 34各自檢出之共振頻率的波形之時間的偏差,可即時檢知 或預測研磨均一性。 〔0127〕 以上,係說明本發明之研磨終點預測方法,所謂與研 磨終點預測相關之共振頻率之波形的特徵變化不限定為變 曲點’包含有上昇開始點、上昇率' 既定的上昇量、及上 昇到下降之變化率等之檢知變化用的共振頻率波形所含有 的所有特徵之項目。 〔0128〕 最後,若要列舉本發明與先前所示之習知公知例在構 成上有大差異的部分時,可列舉以下的相異點: I並非使用將肥粒賴心等磁場作整形的電感器,而是使 用磁場無指向性,在研磨初期依集膚效應積極地不讓磁 場侵入導電性膜内的2次元平面電感器; 2. 將頻率設高到集膚效應可作用的裎度; 3. 針對一次側電感器的形狀或大小、及電感器與除去對象 的導電性膜之㈣,考慮導電性㈣導電率、透磁率並 41 200912252 進行適當化成集膚效應可作用的程度;及 4.考慮基於被研磨對象膜之材質的磁力線之侵入的臨界深 度,設定電感器、頻率、電感器對導電性薄膜的距離。 〔0129〕 習知並没有以集膚效應的影響能顯現那樣的狀態設定 裝置的各要素、故意地基於那樣的集膚效應而形成變曲點 之出現,並依據其而作為監視膜厚來使用者。又,習知中 並未示出巧妙地利用其峰值的存在,將其峰值部分作為膜 厚基準位置而監視膜厚或是算出研磨率等之方法。又,在 習知中所沒有的顯著效果方面,作為渦電流的消耗部分, 有關是在導電性膜被消耗,或是未被導電性膜消耗之下漏 洩到元件,而其成為不被導電性膜消耗的狀態等,透過變 曲點之獲得,能顯著地理解有關磁場對導電性膜侵入的狀 況。以習知的方法而言,被認為不知有關磁場對元件侵入 的狀況,且未考慮磁場的能量對元件之損害,等方面有很 大的差異。本發明係基於根據這樣的明顯不同之作用效果 的差異所搆成的硬體及其檢出計算邏輯者。 〔0130〕 此外,本發明不受上述實施形態所限,係可於本發明 之技術範圍内作各種改變,而且,本發明當然可及於該改 〔圖式簡單說明〕 〔0131〕Nonunif = 〇〇 (%) [0122] Further, in other methods, the film thickness can be removed by subtracting the residual thickness from the initial film thickness, and the unevenness can be obtained by removing the unevenness of the film thickness. [0123] ° or "The unevenness of the amount of polishing may be obtained from the time when the predetermined rate of change (a predetermined amount of polishing) has been reached. [0124] [Formula 10] £ / : The film thickness at the position/removal (·(: the predetermined honing amount at the position of the predetermined change rate at the position/the amount of honing of X is 40 [0125] 200912252 and From (Expression 8) and (Expression 9), the unevenness of the polishing amount can be obtained. 0 [0126] In addition, in FIG. 1, it is shown that an inductor type sensor 34 is disposed on the upper surface of the platform 2. For example, as shown in FIG. 2, a plurality of inductor-type sensors 34 are arranged in a radial direction on the top of the platform 2, and a polishing pad (not shown) is attached to the platform 2, and is simultaneously monitored on the wafer. The waveform of the resonance frequency at each position may also be used. In this case, the deviation of the waveform of the resonance frequency detected from each of the plurality of inductor-type sensors 34 can immediately detect or predict the polishing uniformity. In the above, the polishing end point prediction method of the present invention is described. The characteristic change of the waveform of the resonance frequency related to the polishing end point prediction is not limited to the inflection point 'including the rising start point, the rising rate', the predetermined amount of rise, and the rise. Detection change to the rate of change of decline, etc. Items of all the features included in the resonance frequency waveform used. [0128] Finally, in order to enumerate the parts of the present invention which differ greatly in composition from the conventionally known examples shown in the foregoing, the following differences can be cited: I does not use an inductor that shapes the magnetic field such as the fertiliser, but uses a non-directional magnetic field, and actively removes the magnetic field from the 2-dimensional planar inductor in the conductive film at the initial stage of the polishing; Set the frequency to the temperature at which the skin effect can be applied. 3. Consider the shape or size of the primary inductor, and the conductive film of the inductor and the removed object. Consider conductivity (IV) Conductivity and permeability. 200912252 The degree to which the skin effect can be properly applied; and 4. Consider the critical depth of the intrusion of magnetic lines of force based on the material of the film to be polished, and set the distance between the inductor, the frequency, and the inductor to the conductive film. [0129] It is understood that each element of the state setting device can be visualized by the influence of the skin effect, and the occurrence of the inflection point is intentionally formed based on such a skin effect, and In addition, as a user who monitors the thickness of the film, it is not known to use the peak value as a film thickness reference position to monitor the film thickness or calculate the polishing rate. In terms of significant effects not found in the prior art, as a consuming part of the eddy current, the conductive film is consumed or leaked to the element without being consumed by the conductive film, and it is not consumed by the conductive film. The state of the state, etc., through the acquisition of the inflection point, can clearly understand the state of the magnetic field intrusion into the conductive film. In the conventional method, it is considered that the magnetic field is invaded by the element and the energy of the magnetic field is not considered. There is a large difference in damage to components, etc. The present invention is based on a hardware composed of such distinct effects of the effects and its detection calculation logic. Further, the present invention is not limited to the above-described embodiments, and various changes can be made within the technical scope of the present invention, and the present invention is of course applicable to the modification (a brief description of the drawings) [0131]
1〕顯示本發明的一 實施形態,係化學機械研磨 42 200912252 裝置之斜視圖。 〔囷2(a)〜(c)〕圓2(a)係預測/檢出裴置之方塊圓, 囷2(b)為平面狀電感器之斜視圓,圖2(c)為剖面圓。 〔圖3(a)〜(b)〕圖3(a)係振盪電路之構成解說圖, 囷3 (b)為振盪電路之等價電路圓。 〔圖4(a)〜(d)〕係將預測/檢出裝置之動作模擬結果 顯示於顯示器上的畫像之模式圖,圖4(a)為導體膜厚〇.2 Vm、振盪頻率1MHz的情況,圖4(b)為導體膜厚lym、 振盪頻率1MHz的情況,圖4 (c)為導體膜厚〇.2#m、振 盪頻率40MHz的情況,圖4(d)為導體獏厚iym、振盪頻 率40MHz的情況之圖。 〔圖5〕預測/檢出裝置之等價電路圖。 〔圖6〕預測/檢出裝置之膜厚:阻抗特性的圊表。 〔圖7〕預測/檢出裝置之膜厚:阻抗特性的圊表。 〔圓8〕導體膜上的平面狀電感器之計測點的解說圓。 〔圖9〕顯示圖8之各點的共振頻率波形之一例的圖 表。 〔圖10〕顯示圖8之各點的研磨量之一例的圖表。 〔圊11〕利用本發明之預測/檢出方法研磨Cu膜之際 的參考波形之圖表。 〔囷12〕顯示預測/檢出裝置之其他配置形態的平面 解說圊。 43 200912252 〔主要元件代表符號〕 〔0132〕 1 化學機械研磨ϋ置 2 3 馬達 4 5 研磨墊 6 W 晶圓 28 導電性膜 33預測/檢出裝置 34 35振盪電路 36 36a '41a 基板 33a 37集中常數電容器 38 39 回授網路 40計頻器 41平面狀電感器 L 電感 C0 電容 平臺 驅動機構 研磨頭 電感器型感測器 平面狀電感器 封裴 放大器 441] shows an embodiment of the present invention, which is a perspective view of a chemical mechanical polishing 42 200912252 device. [囷2(a)~(c)] Circle 2(a) is the square circle for predicting/detecting the set, 囷2(b) is the squint circle of the planar inductor, and Fig. 2(c) is the section circle. 3(a) to (b) FIG. 3(a) is a diagram showing the configuration of an oscillation circuit, and 囷3 (b) is an equivalent circuit circle of the oscillation circuit. 4(a) to (d) are schematic diagrams showing an image of an operation simulation result of the prediction/detection device on the display, and Fig. 4(a) shows a conductor film thickness of 22 Vm and an oscillation frequency of 1 MHz. In the case, FIG. 4(b) shows a case where the conductor film thickness is lym and the oscillation frequency is 1 MHz, and FIG. 4(c) shows a case where the conductor film thickness is 2.2#m and the oscillation frequency is 40 MHz, and FIG. 4(d) shows the conductor thickness iym. A diagram of the case where the oscillation frequency is 40 MHz. [Fig. 5] An equivalent circuit diagram of the prediction/detection device. [Fig. 6] Film thickness of the prediction/detection device: a table of impedance characteristics. [Fig. 7] Film thickness of the prediction/detection device: a table of impedance characteristics. [Circle 8] The interpretation circle of the measurement point of the planar inductor on the conductor film. Fig. 9 is a view showing an example of a resonance frequency waveform at each point of Fig. 8. Fig. 10 is a graph showing an example of the amount of polishing at each point of Fig. 8. [圊11] A graph of a reference waveform at the time of polishing a Cu film by the prediction/detection method of the present invention. [囷12] shows the plane explanation of other configurations of the prediction/detection device. 43 200912252 [Main component representative symbol] [0132] 1 Chemical mechanical polishing device 2 3 Motor 4 5 Polishing pad 6 W Wafer 28 Conductive film 33 Prediction/detection device 34 35 Oscillation circuit 36 36a '41a Substrate 33a 37 Concentration Constant Capacitor 38 39 Feedback Network 40 Frequency Counter 41 Planar Inductor L Inductance C0 Capacitor Platform Drive Mechanism Grinding Head Inductor Type Sensor Planar Inductor Sealing Amplifier 44
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