15 research outputs found

    Pataรฑjaliโ€™s Samarthฤhnika

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    ํ•˜ํ”„๋Š„ ์ง€๋ฅด์ฝ”๋Š„ ์ด์‚ฐํ™”๋ฌผ ๋ฐ•๋ง‰์—์„œ์˜ ๋น„์„ ํ˜• wake-up์˜ ๋™์—ญํ•™ ๋ถ„์„

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์‚ฌ๋ฒ”๋Œ€ํ•™ ๊ณผํ•™๊ต์œก๊ณผ(๋ฌผ๋ฆฌ์ „๊ณต),2020. 2. ์ฑ„์Šน์ฒ .Since the discovery of ferroelectricity in Si-doped HfO2 film, numerous studies have been studied based ferroelectric hafnia film. HfO2 based FeRAM is considering as one of the most promising candidate for new type memory devices. Ultra-thin HfO2 film is thermodynamically stable on Si and has robust ferroelectricity properties. Moreover, the remnant polarization (Pr) and ferroelectric coercive field (Ec) are competitive compared with general perovskite ferroelectric materials such as SrBi2Ta2O9 (SBT) and BaTiO3 (BTO). Though Pb(Zr1-xTix)O3 (PZT) is the conventional ferroelectric material, it requires typical thickness of which is >100nm. While that cant match presently with miniaturization tendency on industry, ultra-thin HfO2 film is appropriate for current industry application. However, ferroelectric HfO2 film exhibited an interesting phenomenon as known as the wake-up effect in which remnant polarization increases with the external cycling of the electric field. This wake up effect has been argued with the fact that the phenomenon of redistribution of oxygen vacancies contributes greatly to the expansion of the ferroelectric domain. We report on the nonlinear wake-up behavior against the external electric field cycling in the ferroelectric Hf0.7Zr0.3O2 thin film. Two distinct scaling regimes during the increase of the remnant polarization with different activation energies were observed in TiN/ Hf0.7Zr0.3O2/TiN cells. The transmission electron microscopy revealed the structural phase transition from the monoclinic phase to the orthorhombic phase of the Hf0.7Zr0.3O2 film after the wake-up behavior. During the phase change, as the remnant polarization enhanced, the dielectric constant of the Hf0.7Zr0.3O2 film increased with the external field cycling. The temperature dependence of the wake-up behavior revealed that each estimated activation energies for the early and later enhancement of the remnant polarization are 1.12 eV and 0.73 eV, respectively. First principle calculations show that the oxygen vacancies can reduce the activation energy barrier for the structural phase transition.์‹ค๋ฆฌ์ฝ˜์ด ๋„ํ•‘๋œ HfO2 ๋ฐ•๋ง‰์—์„œ ๊ฐ•์œ ์ „์„ฑ์ด ์ตœ์ดˆ๋กœ ๋ณด๊ณ  ๋œ ์ดํ›„, ๊ฐ•์œ ์ „์ฒด ํ•˜ํ”„๋Š„ ๊ธฐ๋ฐ˜์˜ ๋ฐ•๋ง‰์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ™œ๋ฐœํ•˜๊ฒŒ ์ง„ํ–‰๋˜๊ณ  ์žˆ๋‹ค. HfO2 ๊ธฐ๋ฐ˜์˜ FeRAM์€ ํ˜„์žฌ ์ฐจ์„ธ๋Œ€ ๋ฉ”๋ชจ๋ฆฌ ์†Œ์ž์˜ ๊ฐ€์žฅ ์œ ๋งํ•œ ํ›„๋ณด๋กœ ๊ณ ๋ ค๋˜๊ณ  ์žˆ๋‹ค. HfO2 ๋ฐ•๋ง‰์˜ ๊ฐ•์œ ์ „ ํŠน์„ฑ์€ ์‹ค๋ฆฌ์ฝ˜์—์„œ ์—ด์—ญํ•™์ ์œผ๋กœ ์•ˆ์ •ํ•˜์—ฌ ์ž”๋ฅ˜ ๋ถ„๊ทน ๋ฐ ๊ฐ•์œ ์ „ ๋ณด์ž๋ ฅ ํŠน์„ฑ์ด SrBi2Ta2O9 (SBT) ๋ฐ BaTiO3 (BTO)์™€ ๊ฐ™์€ ์ผ๋ฐ˜์ ์ธ ํŽ˜๋กœ๋ธŒ์Šค์นด์ดํŠธ ๊ฐ•์œ ์ „์„ฑ ์žฌ๋ฃŒ์— ๋น„ํ•ด ๊ฒฝ์Ÿ๋ ฅ์„ ๊ฐ–๋Š”๋‹ค. ์ผ๋ก€๋กœ ์ผ๋ฐ˜์ ์œผ๋กœ ์•Œ๋ ค์ง„ Pb (Zr1-xTix) O3 (PZT)๋Š” ์‹ค๋ฆฌ์ฝ˜์—์„œ ๊ฐ•์œ ์ „ ํŠน์„ฑ์„ ํ™•๋ณดํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” 100nm ์ด์ƒ์˜ ๋‘๊ป˜๋ฅผ ํ•„์š”๋กœ ํ•˜๋ฉฐ ์ด๋Š” ํ˜„์žฌ ์‚ฐ์—…์˜ ์†Œํ˜•ํ™” ํŠธ๋ Œ๋“œ์™€ ๋งž์ง€ ์•Š๋‹ค. ๊ทธ๋Ÿฐ๋ฐ, HfO2๊ธฐ๋ฐ˜ ๊ฐ•์œ ์ „ ๋ฐ•๋ง‰์€ ์ „๊ธฐ์žฅ์˜ ์™ธ๋ถ€ ์‚ฌ์ดํด๋ง์— ์˜ํ•ด ์ž”๋ฅ˜ ๋ถ„๊ตญ์ด ์ฆ๊ฐ€ํ•˜๋Š” "wake-up ํšจ๊ณผ"๋ผ ๋ถˆ๋ฆฌ๋Š” ํฅ๋ฏธ๋กœ์šด ํ˜„์ƒ์ด ๋‚˜ํƒ€๋‚œ๋‹ค. ์ด๋Ÿฌํ•œ wake-up ํšจ๊ณผ๋Š” ์‚ฐ์†Œ ๊ณต๊ทน์˜ ์žฌ๋ถ„๋ฐฐ ํ˜„์ƒ์ด ๊ฐ•์œ ์ „์ฒด ๋„๋ฉ”์ธ ํ™•์žฅ์— ํฌ๊ฒŒ ๊ธฐ์—ฌํ•œ๋‹ค๋Š” ์‚ฌ์‹ค๊ณผ ํ•จ๊ป˜ ์—ฌ๋Ÿฌ ๋…ผ์Ÿ์˜ ์—ฌ์ง€๊ฐ€ ๋‚จ์•„์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ฐ•์œ ์ „ Hf0.7Zr0.3O2 ๋ฐ•๋ง‰์˜ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ ์‚ฌ์ดํด๋ง์— ๋Œ€ํ•œ wake-up ๊ฑฐ๋™์˜ ๋น„์„ ํ˜•์„ฑ์— ๋Œ€ํ•ด ๋ณด๊ณ ํ•œ๋‹ค. TiN / Hf0.7Zr0.3O2 / TiN ๊ตฌ์กฐ์—์„œ ์ž”๋ฅ˜ ๋ถ„๊ทน ๊ฐ’์ด ์ฆ๊ฐ€ํ•˜๋Š” ๋™์•ˆ ์„œ๋กœ ๋‹ค๋ฅธ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋ฅผ ๊ฐ€์ง€๋Š” ๋‘ ๊ฐ€์ง€ ๊ตฌ๋ถ„ ๊ฐ€๋Šฅํ•œ ์˜์—ญ์ด ์žˆ์Œ์„ ํ™•์ธํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๊ณ ํ•ด์ƒ๋„ ํˆฌ๊ณผ ์ „์ž ํ˜„๋ฏธ๊ฒฝ ์‹คํ—˜์„ ํ†ตํ•ด wake-up ๊ฑฐ๋™์ด ์ผ์–ด๋‚œ ํ›„์—๋Š” ๋‹จ์‚ฌ์ •๊ณ„์ƒ์ด ์‚ฌ๋ฐฉ์ •๊ณ„์ƒ์œผ๋กœ ๊ตฌ์กฐ ์ƒ์ „์ด ๋จ์„ ํ™•์ธํ–ˆ๋‹ค. ๊ตฌ์กฐ ์ƒ์ „์ด๋กœ ์ธํ•ด ์™ธ๋ถ€ ํ•„๋“œ ์‚ฌ์ดํด๋ง์— ๋”ฐ๋ผ ์ž”๋ฅ˜ ๋ถ„๊ทน ๊ฐ’์ด์ด ํ–ฅ์ƒ๋˜๋ฉฐ Hf0.7Zr0.3O2 ํ•„๋ฆ„์˜ ์œ ์ „ ์ƒ์ˆ˜๊ฐ€ ํ•จ๊ป˜ ์ฆ์ฆ ํ•˜๋Š” ๊ฒƒ์„ ํ™•์ธํ–ˆ๋‹ค. wake-up ๊ฑฐ๋™์˜ ์˜จ๋„ ์˜์กด์„ฑ ์‹คํ—˜์„ ํ†ตํ•ด wake-up ๊ฑฐ๋™์˜ ์ดˆ๊ธฐ ๋‹จ๊ณ„์™€ ํ›„๊ธฐ ๋‹จ๊ณ„ ์ž”๋ฅ˜ ๋ถ„๊ทน ๊ฐ’ ํ–ฅ์ƒ์— ํ•„์š”ํ•œ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๊ฐ€ ๊ฐ๊ฐ 1.12eV ์™€ 0.73eV ์ธ ๊ฒƒ์„ ํ™•์ธํ–ˆ๋‹ค. ์ œ์ผ์›๋ฆฌ ๊ณ„์‚ฐ์„ ํ†ตํ•ด ์‚ฐ์†Œ ๊ณต๊ทน์ด ๊ตฌ์กฐ ์ƒ์ „์ด์— ๋Œ€ํ•œ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€ ์žฅ๋ฒฝ์„ ์ค„์ผ ์ˆ˜ ์žˆ์Œ์„ ๋ณด์—ฌ์ค€๋‹ค.Abstract 1 Contents 3 List of fugure 4 Introduction 6 Material and methods 8 Results and discussions 9 Conclusion 22 Reference 23 ๊ตญ๋ฌธ์ดˆ๋ก 27 Appendix 29Maste

    โ€˜Guแน‡a-samuddeล›aโ€™ of Bhartแน›hari

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