研究生: |
李健銘 Jian-Ming Li |
---|---|
論文名稱: |
二硫化釕薄膜之雙極式電阻式記憶體 Ruthenium Disulfide Thin Film Based Bipolar Resistive Switching Memory |
指導教授: |
周賢鎧
Shyankay Jou |
口試委員: |
黃柏仁
陳詩芸 |
學位類別: |
碩士 Master |
系所名稱: |
工程學院 - 材料科學與工程系 Department of Materials Science and Engineering |
論文出版年: | 2024 |
畢業學年度: | 112 |
語文別: | 中文 |
論文頁數: | 162 |
中文關鍵詞: | RuS2薄膜 、電阻式記憶體 、硫空缺 、界面型導電機構 、金屬燈絲 |
外文關鍵詞: | RuS2 thin film, resistive memory, sulfur vacancy, interface-type conduction mechanism, metallic filament |
相關次數: | 點閱:108 下載:0 |
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本研究以二硫化釕(Ruthenium disulfide, RuS2)薄膜為介電層應用於電阻式記憶體,製作Ti/RuS2/Ru和Ni/RuS2/Ru元件並比較其電性、切換機構與傳導機制等方面之差異。
Ti/RuS2/Ru元件在電性量測時具有雙極式的電阻切換行為,且在Endurance測試中展現約25倍之開關比。元件在LRS和HRS時皆符合普爾-法蘭克發射機制。在不同電極面積測試中LRS和HRS的電阻值皆會隨電極面積增加而減少,說明此元件屬於界面型導電機構。在升溫測試中LRS和HRS的電阻值會隨溫度升高而下降,為半導體性質,推測元件不是利用燈絲來進行導電,而是利用調整界面能障高低來進行高低電阻態的切換。
Ni/RuS2/Ru元件在電性量測時也具有雙極式的電阻切換行為,且在Endurance測試中展現約10倍之開關比。元件在LRS時皆符合歐姆傳導機制,而在HRS時則符合普爾-法蘭克發射機制。在不同電極面積測試中LRS和HRS的電阻值不隨電極面積改變,說明在LRS是藉由導電燈絲來進行傳導。在升溫測試中HRS的電阻值會隨溫度升高而下降,為半導體性質;LRS的電阻值則會隨溫度升高而增加,為金屬性質,計算之α值與Ni金屬較為接近,因此推測此元件在LRS時是以Ni金屬燈絲作為主要導電燈絲路徑。
Ti/RuS2/Ru元件在I-V量測時僅需0.75 V就可以切換至LRS,-0.85 V切換至HRS;Ni/RuS2/Ru元件則需要1.4 V切換才能至LRS,-1 V切換至HRS,代表界面型導電機構比起金屬導電燈絲機構僅需更小之電壓驅動元件,且只有在界面型導電機構中成功模擬神經元突觸的仿生特性,實現連續電導阻態特性。會有機構上的不同是取決於上電極有無與RuS2薄膜形成中間層,造成RuS2薄膜中的硫空缺增加,有足夠的硫空缺才可調整上電極與RuS2薄膜之間的界面能障高度並進行高低電阻態切換,達成界面型導電機構。
This study applies ruthenium disulfide (RuS2) thin film as the dielectric layer for resistive memory devices. Ti/RuS2/Ru and Ni/RuS2/Ru devices were fabricated, and their electrical characteristics, switching mechanisms, and conduction mechanisms were compared.
The Ti/RuS2/Ru device exhibited bipolar resistive switching behavior during electrical characterization and showed an on/off ratio of around 25 in endurance tests. The device's low resistance state (LRS) and high resistance state (HRS) both followed the Poole-Frenkel emission mechanism. In tests with different electrode areas, the resistance values of both LRS and HRS decreased as the electrode area increased, indicating an interface-type conduction mechanism. In temperature-dependent tests, the resistance values of both LRS and HRS decreased with increasing temperature, suggesting semiconductor-like behavior and implying that the device does not rely on filamentary conduction but rather on modulation of the interface barrier height to achieve resistive switching.
The Ni/RuS2/Ru device also exhibited bipolar resistive switching, with an on/off ratio of around 10 in endurance tests. The LRS followed an ohmic conduction mechanism, while the HRS followed the Poole-Frenkel emission mechanism. The resistance values of both LRS and HRS did not vary with electrode area, suggesting that the LRS is dominated by metallic filamentary conduction. In temperature-dependent tests, the HRS resistance decreased with increasing temperature (semiconductor-like), while the LRS resistance increased with temperature (metallic-like), with the extracted temperature coefficient (α) close to that of Ni, indicating that the main conductive filament in the LRS is likely a Ni metal filament.
Compared to the Ni/RuS2/Ru device, the Ti/RuS2/Ru device requires lower switching voltages (0.75 V to LRS, -0.85 V to HRS) than the Ni/RuS2/Ru device (1.4 V to LRS, -1 V to HRS), indicating that the interface-type conduction mechanism requires lower operating voltages than the metallic filament mechanism. Only the interface-type conduction mechanism successfully mimics the analog synaptic behavior of biological neurons. This difference in mechanism is determined by whether there is an interfacial layer formed between the top electrode and the RuS2 film, which can modulate the sulfur vacancy concentration in the RuS2 film and thus the interface barrier height, enabling the interface-type conduction mechanism.
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