研究生: |
張鈞源 Chun-Yuan Chang |
---|---|
論文名稱: |
複合材料電極濺鍍於鐵電材料之電性研究 Electric Properties of Composite Materials Thin Films on Ferroelectric Materials Prepared by Sputtering |
指導教授: |
周振嘉
Chen-Chia Chou |
口試委員: |
周賢鎧
Shian-Kai Jou 余志成 Jr-Cheng Yu |
學位類別: |
碩士 Master |
系所名稱: |
工程學院 - 機械工程系 Department of Mechanical Engineering |
論文出版年: | 2005 |
畢業學年度: | 93 |
語文別: | 中文 |
論文頁數: | 85 |
中文關鍵詞: | 複合材料 、鐵電材料 、薄膜電極 |
外文關鍵詞: | Composite materials, ferroelectric materials, thin films electrodes |
相關次數: | 點閱:310 下載:1 |
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由於鐵電薄膜多為氧化物,且製程溫度都是在高溫,因此大多搭配使用抗高溫氧化之電極材料作為電極。貴金屬Pt是常使用之材料,然而Pt電極的價格偏高,若能使用較便宜的金屬電極來代替,又能維持導電性,進一步又能降低成本,那麼對元件的製程的成本會大幅的降低,所以本文以Ag電極來取代Pt電極,藉由實驗來了解銀薄膜電極在不同溫度的揮發狀況,試圖匹配緩衝層(buffer Layer )或降低製程溫度和改變製程方法,來了解銀電極應用於鐵電材料的可能性。實驗中並利用XRD、SEM、四點探針,來探討Ag和LSMO-Ag複合材料薄膜電極在不同退火溫度下之薄膜結構、電性以及導電機制。
由實驗結果中, SEM微觀分析知道以銀做為下電極,銀電極在溫度超過300℃時會產生突起現象,且在鍍製LSMO-Ag(1:1)電極時,在鍍膜過程中,銀已開始擴散,雖然在400℃內,複合材料(LSMO-Ag)電極可以防止銀的擴散,但溫度一旦超過400℃時,銀會開始產生團聚突起現象,當溫度超過700℃時,下電極銀在高溫時,開始從未析出區域析出,這說明銀在此溫度開始揮發,也顯示銀含量的多寡,對整個下電極品質的影響有很大的關聯。最後試圖重新配製電極材料成份,以複合材料(LSMO-Ag)來代替純銀電極,並研究此複合材料代替Pt電極後,鐵電材料的特性為何。
研究中發現,電極雖然經過重新的配製後,可以順利量測出鐵電性,而PZT/LSMO-Ag結構在不同溫度退火熱處理後,PZT薄膜的殘留極化值會受到底下基材不同溫度的退火條件而有不同的電性表現,當LSMO-Ag熱處理溫度 600℃時,其PZT的殘留極化值為11.10μC/cm2,而隨著退火溫度增加到700℃∼800℃時,殘留極化值降低到5.50μC/cm2,所以殘留極化值會隨著溫度的上昇而減少。這是因為底電極的LSMO-Ag複合材料中,銀隨著溫度的上昇產生不穩定的擴散與揮發,隨著熱處理溫度的增高,電阻率大幅提升,底電極與PZT的介面擴散越嚴重,造成量測的漏電流越大。
研究最後以CO2雷射退火,來減少底電極與鐵電薄膜在爐管熱處理時,介面所產生的擴散或半導化的問題。PZT薄膜在經由雷射退火後,在底電極熱處理600℃的試片,其殘留極化值Pr約為15.48 μC/cm2,與爐管退火PZT的殘留極化值11.10μC/cm2高,而在底電極熱處理700℃的試片殘留極化值Pr約為14.42 μC/cm2,與爐管退火PZT的殘留極化值7.78μC/cm2比較,其殘留極化值以增加二倍。由此可知,CO2雷射直接能量處理後的試片,已減少內部元素交互擴散的問題,可以改善其元件結構的鐵電特性。
In order to lower the price of the processing, we substitute Ag for Pt as an electrode material. Since most ferroelectric thin films are oxide and the temperature of the processing must be higher, one of the properties of electrode materials must have high-temperature resistance. In this work, we estimate the possibility of applying pure Ag to ferroelectric components by utilizing buffer layer or lower the temperature of the processing, and improve process method. We discuss microstructures, electrical properties and the conductivity mechanism of Ag and Ag-doped LSMO composite thin films through different annealing temperature.
SEM microanalysis shows that diffusion behavior using Ag as bottom electrode is occurred when annealing temperature is beyond 300℃. Also, when we deposit LSMO-Ag(1:1)electrode, Ag begins to diffuse during depositing at the same condition. However, LSMO-Ag electrode is able to prevent the diffusion of Ag under 400℃, but clustering beyond 400℃.When temperature is beyond 700℃, Ag precipitates from non-precipitate-zone. This result represents that the quality of bottom electrode significantly depends on the amount of Ag. Therefore, we attempt to redesign a compatible electrode using LSMO-Ag replacing pure Ag, and study the properties of this composite replacing noble Pt electrode.
During this research, we discovered that we could get ferro-electric ability with our electrode, but after PZT/LSMO-Ag structure annealed under different temperature, remained polarization of PZT would effected by the different material which annealed in the different conditions. When heat treatment were operated under 600 degree Celsius on LSMO-Ag. the remained polarization of PZT were 11.10μC/cm2, when the annealing temperature were up to 700~800, remained polarization were reduced to 5.50μC/cm2, In accordance with it, remained polarization would be reduced when the annealing temperature grow higher. this phenomenon means that when the heat treatment temperature is higher, diffusion would happened in the interface between bottom electrode and PZT, because of the silver in bottom electrode of LSMO-Ag material would unstably diffuse and evaporated, so the leakage current would be detected more when annealing temperature were higher.
In the last part of this research, we would use CO2 laser annealing method to reduce the problem that diffusion and semiconductirization happened between bottom electrode and ferroelectric thin film, and improve the ferroelectric ability of this structure.
After laser annealing method operated on PZT thin film, the remained polarization Pr was 15.48μC/cm2 which the bottom electrodes on substrates heat treated at 600℃. Compared with the substrates which coated PZT on them and heat treated with furnace, remained polarization was 11.10μC/cm2. The remained polarization Pr of the substrates which were heat treated with laser annealing at 700℃ was 14.42μC/cm2, compared with the bottom electrodes which heat treated with furnace, remained polarization was 7.78μC/cm2. So we were informed that laser annealing method operated on substrates could reduce inter diffusion and enhance ferroelectric properties.
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