5 research outputs found

    The Progress of Buddha-land thought of Silla and its historical meanings

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    ν•™μœ„λ…Όλ¬Έ(박사)--μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :ꡭ사학과,2000.Docto

    Study on the Surface-Enhanced Raman Scattering Mechanism and Application to Probing the Surface Potential of Metal Nanostructures

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    1μž₯μ—μ„œλŠ” 기본적인 라만 λΆ„κ΄‘ ν˜„μƒκ³Ό 졜근 λ“€μ–΄ 각광받고 μžˆλŠ” ν‘œλ©΄ 증강 라만 ν˜„μƒ (Surface Enhanced Raman Scattering: SERS) 에 λŒ€ν•΄ κ°„λž΅νžˆ μ†Œκ°œν•˜μ˜€λ‹€. 2μž₯μ—μ„œλŠ” 라만 ν˜„μƒμ˜ 두 λ©”μ»€λ‹ˆμ¦˜ 쀑 ν•˜λ‚˜μΈ μ „μžκΈ° 증강 λ©”μ»€λ‹ˆμ¦˜μ— λŒ€ν•΄ μ—°κ΅¬ν•˜μ˜€λ‹€. 두 개의 금 λ‚˜λ…Έ μž…μž 사이에 1,4-PDI (1,4-phenylenediisocyanide) λΆ„μžλ₯Ό μœ„μΉ˜ν•˜κ²Œ ν•˜μ—¬ λΌλ§Œμ„ μΈ‘μ •ν•˜μ˜€λ‹€. μ‹€ν—˜κ°’κ³Ό FDTD (Finite-difference time domain) 계산방법을 μ΄μš©ν•˜μ—¬ 얻은 κ²°κ³Όλ₯Ό μ΄μš©ν•΄ ν‘œλ©΄ 증강 라만 ν˜„μƒμ˜ 열점 (hot site) 의 크기λ₯Ό λ„μΆœν•΄ λ‚Ό 수 μžˆμ—ˆλ‹€. 10nm 지름을 κ°–λŠ” λ²”μœ„ 내에 μœ„μΉ˜ν•œ μ•½ 400개의 λΆ„μžλ“€μ΄ 전체 라만 μ‹ ν˜Έμ˜ 99%이상에 κΈ°μ—¬ν•œλ‹€λŠ” 사싀을 λ°ν˜”λ‹€. 3.1μž₯μ—μ„œλŠ” ν‘œλ©΄ 증강 라만 ν˜„μƒμ˜ ν™”ν•™ 증강 λ©”μ»€λ‹ˆμ¦˜μ— λŒ€ν•΄ μ—°κ΅¬ν•˜μ˜€λ‹€. ν™”ν•™ 증강 ν˜„μƒμ„ μ΄ν•΄ν•˜κΈ° μœ„ν•΄ 주둜 많이 μ‚¬μš©λ˜μ–΄μ˜¨ 4-ABT (4-aminobenzenethiol) λΆ„μžλ₯Ό 가지고 μ—°κ΅¬ν•˜μ˜€λ‹€. λ¨Όμ € 3.1μž₯μ—μ„œλŠ” ν‘œλ©΄ 증강 ν™œμ„±μ„ κ°–λŠ” 금 κΈ°μ§ˆμ— ν‘μ°©ν•œ 4-ABTλΆ„μžμ˜ b2-type 띠λ₯Ό 주사 λ ˆμ΄μ € 세기와 기질의 μ˜¨λ„μ— 따라 λ³€ν™”ν•˜λŠ” 양상을 κ΄€μΈ‘ν•˜μ˜€λ‹€. κ·Έ κ²°κ³Ό, 4-ABTλΆ„μžκ°€ ν™”ν•™ 증강 ν˜„μƒμ„ λ‚˜νƒ€λ‚΄λŠ” ν™”ν•™ ν™œμ„± 자리둜 μœ„μΉ˜ν•˜κΈ° μœ„ν•΄μ„œλŠ” μž„κ³„ μ—λ„ˆμ§€ μ΄μƒμ˜ μ—λ„ˆμ§€κ°€ ν•„μš”ν•˜λ‹€λŠ” λͺ¨λΈμ„ μ„Έμš°κ²Œ λ˜μ—ˆλ‹€. 3.2μž₯μ—μ„œλŠ” μ§€κΈˆκΉŒμ§€ 4-ABTλΆ„μžμ—μ„œλ§Œ κ΄€μΈ‘λ˜μ–΄μ˜¨ b2-type의 띠듀이 4-ABT 뿐만 μ•„λ‹ˆλΌ λ‹€μ–‘ν•œ 4-ABT μœ λ„μ²΄ λΆ„μžλ“€μ—μ„œλ„ λ™μΌν•˜κ²Œ 관츑됨을 λ°ν˜”λ‹€. λ¨Όμ €, 4-BDBT (4-(benzylideneamino)benzenethiol) λΆ„μžμ™€ 4-DMABT (4-(diethylamino)benzenethiol) λΆ„μžλ₯Ό μ΄μš©ν•΄ b2-type의 띠듀이 μƒμ„±λ˜λŠ” 것이 κ΄‘λ°˜μ‘κ³ΌλŠ” 상관이 μ—†λŠ” ν˜„μƒμž„μ„ λ°ν˜”λ‹€. 그리고 λ‹€μ–‘ν•œ 4-ABTμœ λ„μ²΄ λΆ„μžλ“€μ˜ μ „κ·Ήμ „μœ„μ˜μ‘΄ ν‘œλ©΄ 증강 라만 μ‹€ν—˜μ„ 톡해 b2- type의 띠듀이 λͺ¨λ‘ λΉ„μŠ·ν•œ νŠΉμ„±μ„ 가짐을 ν™•μΈν•˜μ˜€λ‹€. 4μž₯μ—μ„œλŠ” κ·Ήμ„± 유기 휘발 μš©λ§€μ— λŒ€ν•œ 금 λ‚˜λ…Έ μž…μžμ˜ ν‘œλ©΄ μ „μœ„ λ³€ν™”λ₯Ό ν‰ν‰ν•œ 금 μ „κ·Ή μœ„μ— 금 λ‚˜λ…Έ μž…μžλ‘œ 이루어진 ν‹ˆμ— μœ„μΉ˜ν•œ 1,4-PDI λΆ„μžλ₯Ό μ΄μš©ν•΄ κ°μ§€ν•˜λŠ” κΈ°μˆ μ„ κ°œλ°œν•˜μ˜€λ‹€. μ „κ·Ή μ „μœ„ 의쑴 ν‘œλ©΄μ¦κ°•λΌλ§Œ 츑정을 톡해, μ „μœ„ 아세톀과 μ•”λͺ¨λ‹ˆμ•„λ₯Ό ν˜λ €μ£Όμ—ˆμ„ λ•Œμ˜ 금 λ‚˜λ…Έ μž…μžμ˜ ν‘œλ©΄μ „μœ„κ°€ 포화 AgAgCl μ „κ·Ήκ³Ό 비ꡐ해볼 λ•Œ +0.7 V μ—μ„œ -0.6 VκΉŒμ§€ λ³€ν™”ν•œλ‹€λŠ” 사싀을 확인할 수 μžˆμ—ˆλ‹€.Chapter 1 describes general introduction of the thesis. Classical Raman Scattering and Surface-enhanced Raman scattering (SERS) Spectroscopy are introduced briefly. In Chapter 2, I estimated the size of hot sites for SERS located within the gap between two 1,4-phenylene diisocyanide-incorporated Au nanoparticles by using both Raman experiment and finite-difference time-domain calculation. About 400 molecules residing within a 10-nm diameter area of the center of the gap irradiated by a laser light, must contribute more than 99% to the total Raman signal of 1,4-phenylene diisocyanide. This apparently indicates that the size of hot site is very limited. In Chapter 3.1, temperature dependent Raman scattering measurements were conducted for 4-aminobenzenethiol adsorbed on the gold surface. It was verified that some threshold energy is required for 4-aminobenzenethiol to occupy the gold surface sites capable of leading to the appearance of surface-enhanced Raman scattering peaks via a charge transfer resonance enhancement mechanism. In Chapter 3.2, it is examined the SERS spectral pattern of various 4-aminobenzenethiol derivatives adsorbed on Ag substrates. At first, is is found in the SERS spectra of 4-(diethylamino)benzenethiol and 4-(benzylideneamino)benzenethiol that no photoreaction had taken place at all but the b2-type bands appeared distinctly as is usual in the SERS of 4-ABT. The b2-type bands were also observed in the SERS spectra of other 4-ABT derivatives while, surprisingly, no such b2-type bands were observed at all in the SERS spectra of para-substituted (but not amino) benzenethiol derivatives. The appearance of the b2-type bands in the SERS spectra seemed thus a common feature of 4-ABT derivatives. The difference between 4-ABT derivatives and para-substituted (but not amino) benzenethiol derivatives was supposedly associated with the LUMO-HOMO energy gap. The energy gap computed for 4-ABT derivatives (~300 nm) was consonant with the interpretation that the appearance of the b2-type bands in the SERS spectrum of 4-ABT is associated with an intensity borrowing from an intense * molecular transition (1A1 1B2) at 300 nm. In Chapter 4, large peak shift was observed for the NC stretching band of 1,4-phenylene diisocyanide (1,4-PDI) situated at the gap between gold nanoparticles and gold electrode when gold nanoparticles are exposed to polar organic solvent like acetone and ammonia. The peak shift amounted to as much as 22 cm-1, corresponding to the variation of surface potential of Au nanoparticles from +0.7 V to -0.6 V vs a saturated Ag/AgCl electrode. The peak shift observed in this work must be due to the large surface-to-volume ratio of Au nanoparticlesDocto

    Fabrication of various nanotextured materials and relaxation dynamics of TiOβ‚‚Ag nanocomposite systems

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    Thesis (master`s)--μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :ν™”ν•™λΆ€ 물리화학전곡,2004.Maste

    A Study on the Historical Transition and Significance of Cheongryeonsa Temple

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