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    ์ „๊ธฐ์žฅ์„ ์ด์šฉํ•œ ๋ถ„์ž ๋ฐ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ ์กฐ์ž‘์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ํ™”ํ•™๋ถ€,2020. 2. ๊ฐ•ํ—Œ.This dissertation aims to demonstrate how a strong external electrostatic field on the order of 10^8 V/m manipulates molecular properties, such as orientation, structure, dynamics, etc., of small molecules and molecular clusters isolated in cold inert matrices. A combination of the ice film nanocapacitor method and the matrix isolation technique enabled the application of unprecedentedly intense external electric dc fields across the isolated molecules and molecular clusters. Changes in molecular properties driven by external fields were investigated by means of vibrational spectroscopy. Chapter 1 provides a background of molecular-control studies with external forces. A brief history of molecular manipulation using electrostatic, magnetic, and optical fields is introduced, with more detailed examples on molecular control with electrostatic fields in both gas-phase and condensed-phase molecular systems. A concise introduction to the methodology of research in the present dissertation is also given. Detailed experimental methods are described in Chapter 2. The fundamentals and practical aspects of the ice film nanocapacitor method for applying intense external fields, the matrix isolation technique for preparing isolated molecular species, and the reflectionโ€“absorption infrared spectroscopy for detecting molecular behaviors are summarized. A description on the instrumentation used in the experiments is provided. Chapter 3 presents the spectroscopic study on the field-driven change in inversion tunneling dynamics of ammonia molecule. An ammonia molecule isolated in the Ar matrix, which undergoes a rapid umbrella inversion tunneling across the barrier of the symmetric double-minimum potential energy surface when undisturbed, reorients into the direction of an strong external field by Stark mixing of inversion states with close energy levels and opposite parities. An external field results in the asymmetrization of the double-minimum potential and thereby the quenching of inversion dynamics. The static infrared spectra recorded at systematically scanned-field strengths, which encrypt such field-induced behavior of ammonia, were decoded with the help of potential energy surface, localization of wavefunctions, and transition selection rule under the external dc field. Chapter 4 reports the experimental measurement of the vibrational Stark sensitivity of small hydrogen-bonded water and ammonia clusters ((D2O)3, (D2O)4, (NH3)3, NH3โ€“HCl, NH3โ€“H2O, and (ND3)3). The vibrational Stark effect manifests the frequency shift as a result of the field-induced manipulation of potential energy surfaces of molecular vibrations. The Stark sensitivity of vibrations of the clusters was found to significantly differ from the corresponding uncomplexed monomer. The clustering effect on the Stark sensitivity is discussed in the perspective of anharmonicity, geometric effect, and intermolecular vibrational coupling. As an extreme example of the clustering through hydrogen-bonding, Stark spectra of a crystalline ice were qualitatively interrogated and compared with those of the isolated water monomer. Chapters 5 and 6 demonstrate that a strong electrostatic field enables the dislocation of an acidic proton. In Chapter 5, vibrational Stark spectroscopy was conducted for hydrogen chlorideโ€“water (HClโ€“H2O, HClโ€“D2O) complexes to examine the field-induced behavior of the proton in hydrated acids. The spectra of the complexes showed an extraordinarily large Stark shift of the proton stretching frequency compared to that of uncomplexed HCl molecule. In the case of HClโ€“D2O, the vibrational coupling between the proton stretching and the symmetric stretching of D2O was modified by external fields. Spectral analysis aided by a quantum calculation reveals the reversible and asymmetric translocation of the acidic proton along the proton-transfer coordinate in the HClโ€“water complexes by applied fields. Chapter 6 reports the Stark spectra of HCl complexes with ammonia and methylated amines (methylamine, dimethylamine, and trimethylamine), a prototypical example of proton-transferring molecular system. Not only the proton stretching vibration which is a parallel/anti-parallel motion of proton along the proton-transfer coordinate but also the perpendicular proton bending mode showed exceptionally drastic spectral changes under the influence of external fields. The spectral changes by fields were characteristic of each complex with different degree of proton transfer. The studies on the hydrated acids and the proton-transfer complexes provide the spectroscopic evidence of the large protonic polarizability, a concept which occupies a prominent position in the behavior and spectroscopy of proton in chemistry. Chapter 7 summarizes the dissertation. The significance and prospect of the research presented in this dissertation are briefly addressed in the perspective of intermolecular processes in chemistry and molecular manipulation in quantum technology.๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์€ 10^8 V/m ์ˆ˜์ค€์˜ ๊ฐ•ํ•œ ์™ธ๋ถ€ ์ •์ „๊ธฐ์žฅ์ด ์ €์˜จ์˜ ๋น„ํ™œ์„ฑ ๋งคํŠธ๋ฆญ์Šค ๋‚ด์— ๊ณ ๋ฆฝ๋œ ๋ถ„์ž ๋ฐ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ์˜ ๋ฐฉํ–ฅ, ๊ตฌ์กฐ, ๋™๋ ฅํ•™ ๋“ฑ์˜ ์„ฑ์งˆ์„ ์–ด๋–ป๊ฒŒ ์กฐ์ž‘ํ•˜๋Š”์ง€์— ๋Œ€ํ•ด ๋‹ค๋ฃฌ๋‹ค. ์–ผ์Œ ๋ฐ•๋ง‰ ์ถ•์ „๋ฒ•๊ณผ ๋งคํŠธ๋ฆญ์Šค ๊ณ ๋ฆฝ๋ฒ•์„ ๋™์‹œ์— ์ด์šฉํ•˜์—ฌ ์ด์ „ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ฐ€ํ•  ์ˆ˜ ์—†์—ˆ๋˜ ๊ฐ•ํ•œ ์™ธ๋ถ€ ์ง๋ฅ˜ ์ „๊ธฐ์žฅ์„ ๊ณ ๋ฆฝ๋œ ๋ถ„์ž์™€ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ์— ๊ฐ€ํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์— ์˜ํ•œ ๋ถ„์ž ํŠน์„ฑ์˜ ๋ณ€ํ™”๋Š” ์ง„๋™ ๋ถ„๊ด‘ํ•™์„ ์ด์šฉํ•ด ๊ด€์ธกํ•˜์˜€๋‹ค. 1์žฅ์—์„œ๋Š” ์™ธ๋ถ€ ํž˜์„ ํ†ตํ•ด ๋ถ„์ž๋ฅผ ์กฐ์ž‘ํ•˜๋Š” ๊ธฐ์กด ์—ฐ๊ตฌ๋“ค์„ ์†Œ๊ฐœํ•œ๋‹ค. ์ •์ „๊ธฐ์žฅ, ์ž๊ธฐ์žฅ, ๊ด‘ํ•™ ์ „๊ธฐ์žฅ ๋“ฑ์˜ ์™ธ๋ถ€ ํž˜์„ ์ด์šฉํ•œ ๋ถ„์ž ์กฐ์ž‘์— ๊ด€ํ•œ ๊ฐ„๋‹จํ•œ ์—ญ์‚ฌ๋ฅผ ์†Œ๊ฐœํ•˜๊ณ , ๊ทธ ํ›„์—๋Š” ์ •์ „๊ธฐ์žฅ์„ ์ด์šฉํ•œ ์—ฐ๊ตฌ๋“ค์— ๋Œ€ํ•ด ๋ณด๋‹ค ์ž์„ธํžˆ ๋‹ค๋ฃฌ๋‹ค. ๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ ์—ฐ๊ตฌ์—์„œ ์ด์šฉ๋œ ๋ฐฉ๋ฒ•๋ก ์— ๋Œ€ํ•ด์„œ๋„ ๊ฐ„๋‹จํžˆ ์†Œ๊ฐœํ•œ๋‹ค. 2์žฅ์—์„œ๋Š” ์—ฐ๊ตฌ์— ์‚ฌ์šฉ๋œ ์‹คํ—˜ ๋ฐฉ๋ฒ•์„ ์„ค๋ช…ํ•œ๋‹ค. ๊ฐ•ํ•œ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์„ ๊ฑธ์–ด์ฃผ๊ธฐ ์œ„ํ•ด ์–ผ์Œ ๋ฐ•๋ง‰ ์ถ•์ „๋ฒ•์„ ์‚ฌ์šฉํ•˜์˜€๊ณ , ๊ณ ๋ฆฝ๋œ ๋ถ„์ž ๋ฐ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ๋ฅผ ๋งŒ๋“ค๊ธฐ ์œ„ํ•ด์„œ๋Š” ๋งคํŠธ๋ฆญ์Šค ๊ณ ๋ฆฝ๋ฒ•์„ ์‚ฌ์šฉํ•˜์˜€๋‹ค. ์ „๊ธฐ์žฅ์— ์˜ํ•œ ๋ถ„์ž ๋ฐ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ์˜ ๋ณ€ํ™”๋Š” ๋ฐ˜์‚ฌ-ํก์ˆ˜ ์ ์™ธ์„  ๋ถ„๊ด‘๋ฒ•์ด ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ์ด ๋ฐฉ๋ฒ•๋“ค์— ๋Œ€ํ•œ ์›๋ฆฌ์ , ์‹ค์šฉ์  ์ธก๋ฉด๋“ค์„ ์š”์•ฝํ•œ๋‹ค. ์‹คํ—˜์— ์‚ฌ์šฉ๋œ ์žฅ์น˜์— ๋Œ€ํ•ด์„œ๋„ ๋ฌ˜์‚ฌํ•œ๋‹ค. 3์žฅ์€ ์•”๋ชจ๋‹ˆ์•„ ๋ถ„์ž์˜ ๋ฐ˜์ „ ํ„ฐ๋„๋ง ๋™๋ ฅํ•™์˜ ์ „๊ธฐ์žฅ์— ์˜ํ•œ ๋ณ€ํ™”์— ๋Œ€ํ•œ ๋ถ„๊ด‘ํ•™์  ์—ฐ๊ตฌ์ด๋‹ค. ์•„๋ฅด๊ณค ๋งคํŠธ๋ฆญ์Šค ๋‚ด์˜ ์•”๋ชจ๋‹ˆ์•„ ๋ถ„์ž๋Š” ์™ธ๋ถ€ ๋ฐฉํ•ด๊ฐ€ ์—†์„ ๋•Œ ๋Œ€์นญ์ ์ธ ์ด์ค‘-์ตœ์†Œ์  ํผํ…์…œ ์—๋„ˆ์ง€ ํ‘œ๋ฉด ๋‚ด์—์„œ ๋งค์šฐ ๋น ๋ฅธ ์šฐ์‚ฐ-๋ฐ˜์ „ ํ„ฐ๋„๋ง์„ ์ผ์œผํ‚ค๋Š” ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ๋‹ค. ๊ฐ•ํ•œ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์ด ๊ฐ€ํ•ด์ง€๋ฉด ๋ฐ˜์ „ ์ƒํƒœ๋“ค์˜ Stark ์„ž์ž„์ด ์ผ์–ด๋‚˜๊ณ , ๊ทธ๋กœ์ธํ•ด ๋ถ„์ž๊ฐ€ ์ „๊ธฐ์žฅ ๋ฐฉํ–ฅ์œผ๋กœ ์ •๋ ฌํ•˜๊ฒŒ ๋œ๋‹ค. ์ •๋ ฌ๋œ ์•”๋ชจ๋‹ˆ์•„ ๋ถ„์ž๋Š” ๋น„๋Œ€์นญ์ ์ธ ์ด์ค‘-์ตœ์†Œ์  ํผํ…์…œ ์—๋„ˆ์ง€ ํ‘œ๋ฉด์„ ๊ฐ€์ง€๊ฒŒ ๋˜๊ณ , ๋”ฐ๋ผ์„œ ๋ฐ˜์ „ ํ„ฐ๋„๋ง์ด ์ผ์–ด๋‚˜์ง€ ์•Š๊ฒŒ ๋œ๋‹ค. ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์— ์˜ํ•œ ์ด๋Ÿฌํ•œ ๋ณ€ํ™”๋“ค์€ ์ „๊ธฐ์žฅ ์„ธ๊ธฐ๋ฅผ ๋ณ€ํ™”์‹œ์ผœ๊ฐ€๋ฉฐ ์–ป์€ ์ ์™ธ์„  ์ŠคํŽ™ํŠธ๋Ÿผ์— ์•”ํ˜ธํ™”๋˜์–ด ์žˆ์œผ๋ฉฐ, ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ํผํ…์…œ ์—๋„ˆ์ง€ ํ‘œ๋ฉด, ํŒŒ๋™ํ•จ์ˆ˜์˜ ํŽธ์žฌํ™”, ์ „์ด ์„ ํƒ ๊ทœ์น™ ๋“ฑ์„ ์ด์šฉํ•˜์—ฌ ์ด๋ฅผ ํ•ด์„ํ•˜์˜€๋‹ค. 4์žฅ์—์„œ๋Š” ๋ฌผ๊ณผ ์•”๋ชจ๋‹ˆ์•„ ๋ถ„์ž๋ฅผ ํฌํ•จํ•˜๋Š” ์ˆ˜์†Œ ๊ฒฐํ•ฉ ํด๋Ÿฌ์Šคํ„ฐ์˜ ์ง„๋™ Stark ๋ฏผ๊ฐ๋„์˜ ์‹คํ—˜์  ์ธก์ •์— ๊ด€ํ•ด ๋‹ค๋ฃฌ๋‹ค. ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์€ ๋ถ„์ž ์ง„๋™์˜ ํผํ…์…œ ์—๋„ˆ์ง€ ํ‘œ๋ฉด์„ ์กฐ์ž‘ํ•˜์—ฌ ์ง„๋™์ˆ˜ ์ด๋™์„ ์ผ์œผํ‚ค๋Š”๋ฐ, ์ด๋ฅผ ์ง„๋™ Stark ํšจ๊ณผ๋ผ๊ณ  ํ•œ๋‹ค. ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ์˜ ์ง„๋™ Stark ๋ฏผ๊ฐ๋„๋Š” ํด๋Ÿฌ์Šคํ„ฐ๋ฅผ ์ด๋ฃจ์ง€ ์•Š์€ ๋‹จ๋… ๋ถ„์ž์˜ ๋ฏผ๊ฐ๋„์™€ ํฌ๊ฒŒ ๋‹ค๋ฅธ ๊ฒƒ์œผ๋กœ ๊ด€์ฐฐ๋˜์—ˆ๋‹ค. ์ด๋Ÿฌํ•œ ํด๋Ÿฌ์Šคํ„ฐ ํšจ๊ณผ๋ฅผ ์ง„๋™์˜ ๋น„์กฐํ™”์„ฑ, ๊ตฌ์กฐ์  ํšจ๊ณผ, ๋ถ„์ž๊ฐ„ ์ง„๋™ ์ง์ง€์Œ ๋“ฑ์˜ ์ธก๋ฉด์—์„œ ๋…ผ์˜ํ•œ๋‹ค. ์ˆ˜์†Œ ๊ฒฐํ•ฉ์„ ํ†ตํ•œ ํด๋Ÿฌ์Šคํ„ฐ๋ง์˜ ๊ทน๋‹จ์  ์˜ˆ์‹œ๋กœ ๊ฒฐ์ •ํ˜• ์–ผ์Œ์˜ ์ง„๋™ ์ŠคํŽ™ํŠธ๋Ÿผ์ด ์ „๊ธฐ์žฅ์— ์˜ํ•ด ์–ด๋–ป๊ฒŒ ๋ณ€ํ•˜๋Š”์ง€๋ฅผ ์กฐ์‚ฌํ•˜์˜€์œผ๋ฉฐ, ์ด๋ฅผ ๋‹จ๋… ๋ฌผ๋ถ„์ž์™€ ๋น„๊ตํ•˜์˜€๋‹ค. 5์žฅ๊ณผ 6์žฅ์€ ๊ฐ•ํ•œ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์ด ์‚ฐ์„ฑ ์–‘์„ฑ์ž๋ฅผ ์ด๋™์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค๋Š” ๊ฒƒ์„ ์‹คํ—˜์ ์œผ๋กœ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. 5์žฅ์€ ์—ผํ™”์ˆ˜์†Œ-๋ฌผ(H2O, D2O) ํด๋Ÿฌ์Šคํ„ฐ์— ๋Œ€ํ•œ ์ง„๋™ Stark ๋ถ„๊ด‘ํ•™์  ์—ฐ๊ตฌ์ด๋‹ค. ์ด ํด๋Ÿฌ์Šคํ„ฐ์˜ ์–‘์„ฑ์ž ์‹ ์ถ• ์ง„๋™์ˆ˜๊ฐ€ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์— ์˜ํ•ด ๋งค์šฐ ํฌ๊ฒŒ ๋ณ€ํ™”ํ•œ ๊ฒƒ์„ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ์—ผํ™”์ˆ˜์†Œ-D2O ํด๋Ÿฌ์Šคํ„ฐ์˜ ๊ฒฝ์šฐ์—๋Š” ์–‘์„ฑ์ž ์‹ ์ถ• ์ง„๋™๊ณผ D2O์˜ ๋Œ€์นญ ์‹ ์ถ• ์ง„๋™์˜ ์ง์ง€์Œ์ด ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์— ์˜ํ•ด ๋ณ€ํ•˜๋Š” ๊ฒƒ์„ ๊ด€์ฐฐํ•˜์˜€๋‹ค. ์–‘์ž ๊ณ„์‚ฐ์„ ์ด์šฉํ•ด ์ŠคํŽ™ํŠธ๋Ÿผ์„ ํ•ด์„ํ•œ ๊ฒฐ๊ณผ, ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์ด ์—ผํ™”์ˆ˜์†Œ- ๋ฌผ ํด๋Ÿฌ์Šคํ„ฐ์˜ ์–‘์„ฑ์ž ์ „๋‹ฌ ์ขŒํ‘œ ์ƒ์—์„œ ์–‘์„ฑ์ž๊ฐ€ ๊ฐ€์—ญ์ , ๋น„๋Œ€์นญ์ ์œผ๋กœ ์ด๋™ํ•˜๋„๋ก ์œ ๋„ํ•œ๋‹ค๋Š” ์‚ฌ์‹ค์„ ์•Œ ์ˆ˜ ์žˆ์—ˆ๋‹ค. 6์žฅ์€ ์—ผํ™”์ˆ˜์†Œ์™€ ์•”๋ชจ๋‹ˆ์•„, ๋ฉ”ํ‹ธํ™”๋œ ์•„๋ฏผ ๋ถ„์ž์˜ ํด๋Ÿฌ์Šคํ„ฐ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ์ด๋‹ค. ์ด ํด๋Ÿฌ์Šคํ„ฐ๋“ค์€ ์–‘์„ฑ์ž ์ „๋‹ฌ ์‹œ์Šคํ…œ์˜ ๋Œ€ํ‘œ์ ์ธ ์˜ˆ์ด๋‹ค. ํ‰ํ–‰ํ•œ ๋ฐฉํ–ฅ์˜ ์–‘์„ฑ์ž ์‹ ์ถ• ์ง„๋™ ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ์ˆ˜์ง ๋ฐฉํ–ฅ์˜ ์–‘์„ฑ์ž ๊ตฝํž˜ ์ง„๋™ ์—ญ์‹œ ์™ธ๋ถ€ ์ „๊ธฐ์žฅ์— ์˜ํ•ด ํฐ ์ง„๋™์ˆ˜ ๋ณ€ํ™”๋ฅผ ๋‚˜ํƒ€๋ƒˆ๋‹ค. ๊ฐ ์–‘์„ฑ์ž ์ „๋‹ฌ ๋ถ„์ž ํด๋Ÿฌ์Šคํ„ฐ๋Š” ์ „๊ธฐ์žฅ์— ์˜ํ•ด ๊ณ ์œ ํ•œ ์ŠคํŽ™ํŠธ๋Ÿผ ๋ณ€ํ™”๋ฅผ ๋ณด์˜€๋‹ค. ์ˆ˜ํ™”๋œ ์‚ฐ์„ฑ ๋ถ„์ž์™€ ์–‘์„ฑ์ž ์ „๋‹ฌ๊ณ„์— ๋Œ€ํ•œ ์ด๋Ÿฌํ•œ ์—ฐ๊ตฌ๋Š” ์–‘์„ฑ์ž์˜ ๊ฑฐ๋™์— ์žˆ์–ด์„œ ํ•ต์‹ฌ์ ์ธ ๊ฐœ๋…์ธ ํฐ ์–‘์„ฑ์ž ํŽธ๊ทน๋„์— ๋Œ€ํ•œ ์‹คํ—˜์  ์ฆ๊ฑฐ๋ฅผ ์ œ๊ณตํ•œ๋‹ค. 7์žฅ์€ ๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์˜ ์š”์•ฝ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์˜ ์ค‘์š”์„ฑ๊ณผ ์ „๋ง์„ ๋ถ„์ž๊ฐ„ ํ™”ํ•™์  ๊ณผ์ •๊ณผ ์–‘์ž ๊ธฐ์ˆ ์—์„œ์˜ ๋ถ„์ž ์กฐ์ž‘์˜ ์ธก๋ฉด์—์„œ ์„œ์ˆ ํ•œ๋‹ค.Chapter 1. Introduction 1 1.1. Manipulation of Molecules with External Fields 2 1.2. Manipulation of Molecules with Homogeneous Electrostatic Fields 4 1.3. Approach and Contents of This Dissertation 6 References 8 Chapter 2. Method 16 2.1. A Combined Technique of Ice Film Nanocapacitor and Matrix Isolation 16 2.2. Reflection-Absorption Infrared Spectroscopy of Matrix-Isolated Molecules under the Influence of External Fields 21 2.3. Instruments 24 References 27 Chapter 3. Electric Field-Control of Inversion Dynamics of Ammonia in an Argon Matrix 31 Abstract 31 3.1. Introduction 32 3.2. Experimental Details 34 3.3. Results and Discusstion 35 3.4. Conclusion 47 References 49 Chapter 4. Experimental Measurement of Vibrational Stark Sensitivity of Small Molecular Clusters: Clustering Effect on Stark Response of Vibrations 52 Abstract 52 4.1. Introduction 53 4.2. Experimental Details 55 4.3. Results and Discussion 56 4.4. Conclusion 70 References 71 Chapter 5. Spectroscopic Evidence of Large Protonic Polarizability of Hydrogen Chloride-Water Complexes 77 Abstract 77 Main Text 78 References 88 Supporting Information 92 Chapter 6. Vibrational Stark Spectroscopy on Proton Vibrations in Proton-Transfer Complexes of Hydrogen Chloride with Ammonia and Methylated Amines 103 Abstract 103 6.1. Introduction 104 6.2. Experimental Details 107 6.3. Results 108 6.4. Discussion 115 6.5. Conclusion 121 References 122 Chapter 7. Summary 126 List of Publications 128 Abstract in Korean (๊ตญ๋ฌธ ์ดˆ๋ก) 131 Acknowledgement (๊ฐ์‚ฌ์˜ ๊ธ€) 135Docto

    Theoretical Studies of Spectroscopy and Dynamics of Hydrated Electrons.

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    Solar and Stellar Photospheric Abundances

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    The determination of photospheric abundances in late-type stars from spectroscopic observations is a well-established field, built on solid theoretical foundations. Improving those foundations to refine the accuracy of the inferred abundances has proven challenging, but progress has been made. In parallel, developments on instrumentation, chiefly regarding multi-object spectroscopy, have been spectacular, and a number of projects are collecting large numbers of observations for stars across the Milky Way and nearby galaxies, promising important advances in our understanding of galaxy formation and evolution. After providing a brief description of the basic physics and input data involved in the analysis of stellar spectra, a review is made of the analysis steps, and the available tools to cope with large observational efforts. The paper closes with a quick overview of relevant ongoing and planned spectroscopic surveys, and highlights of recent research on photospheric abundances.Comment: Invited review to appear in Living Reviews in Solar Physics. 39 pages, 7 figure

    Development of innovative analytical methods based on spectroscopic techniques and multivariate statistical analysis for quality control in the food and pharmaceutical fields.

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    The increasing demand on quality assurance and ever more stringent regulations in food and pharmaceutical fields are promoting the need for analytical techniques enabling to provide reliable and accurate results. However, traditional analytical methods are labor-intensive, time-consuming, expensive and they usually require skilled personnel for performing the analysis. For these reasons, in the last decades, quality control protocols based on the employment of spectroscopic methods have been developed for many different application fields, including pharmaceutical and food ones. Vibrational spectroscopic techniques can be an adequate alternative for acquiring both chemical and physical information related to homogenous and heterogenous matrices of interest. Moreover, the significant development of powerful data-driven methodologies allowed to develop algorithms for the optimal extraction and processing of the complex spectroscopic signals allowing to apply combined approaches for quantitative and qualitative purposes. The present Doctoral Thesis has been focused on the development of ad-hoc analytical strategies based on the application of spectroscopic techniques coupled with multivariate data analysis approaches for providing alternative analytical protocols for quality control in food and pharmaceutical sectors. Regarding applications in food sector, excitation-emission Fluorescence Spectroscopy, Near Infrared Spectroscopy (NIRS) and NIR Hyperspectral Imaging (HSI) have been tested for solving analytical issues of independent case-studies. Unsupervised approaches based on Principal Component Analysis (PCA) and Parallel Factor Analysis (PARAFAC) have been applied on fluorescence data for characterizing green tea samples, while quantitative predictive approaches as Partial Least Squares regression have been used to correlate NIR spectra with quality parameters of extra-virgin olive oil samples. HSI was applied to study dynamic chemical processes which occur during cheese ripening with the aim to map chemical and sensory changes over time. The rapid technical progress in terms of spectroscopic instrumentations has led to have more flexible portable systems suitable for performing measurements directly in the field or in a manufacturing plant. Within this scenario, NIR spectroscopy proved to be one of the most powerful Process Analytical Technologies (PAT) for monitoring and controlling complex manufacturing processes. In this thesis, two applications based on the implementation of miniaturized NIR sensors have been performed for the real-time powder blending monitoring of pharmaceutical and food formulation, respectively. The main challenges in blending monitoring are related to the assessment of the homogeneity of multicomponent formulations, which is crucial to ensure the safety and effectiveness of a solid pharmaceutical formulation or the quality of a food product. In the third chapter of this thesis, tailor made qualitative chemometric strategies for obtaining a global understanding of blending processes and to optimize the endpoint detection are presented

    Influence of subunit structure on the oligomerization state of light harvesting complexes: a free energy calculation study

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    Light harvesting complexes 2 (LH2) from Rhodospirillum (Rs.) molischianum and Rhodopseudomonas (Rps.) acidophila form ring complexes out of eight or nine identical subunits, respectively. Here, we investigate computationally what factors govern the different ring sizes. Starting from the crystal structure geometries, we embed two subunits of each species into their native lipid-bilayer/water environment. Using molecular dynamics simulations with umbrella sampling and steered molecular dynamics, we probe the free energy profiles along two reaction coordinates, the angle and the distance between two subunits. We find that two subunits prefer to arrange at distinctly different angles, depending on the species, at about 42.5 deg for Rs. molischianum and at about 38.5 deg for Rps. acidophila, which is likely to be an important factor contributing to the assembly into different ring sizes. Our calculations suggest a key role of surface contacts within the transmembrane domain in constraining these angles, whereas the strongest interactions stabilizing the subunit dimers are found in the C-, and to a lesser extent, N-terminal domains. The presented computational approach provides a promising starting point to investigate the factors contributing to the assembly of protein complexes, in particular if combined with modeling of genetic variants.Comment: 28 pages, 7 figures, LaTeX2e - requires elsart.cls (included), submitted to Chemical Physic

    Assessment of Multi-Scale Approaches for ComputingUVโ€“Vis Spectra in Condensed Phases: Toward an Effective yetReliable Integration of Variational and Perturbative QM/MM Approaches

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    Computational simulation of UV/vis spectra in condensed phases can be performed starting from converged molecular dynamics (MD) simulations and then performing quantum mechanical/molecular mechanical (QM/MM) computations for a statistically significant number of snapshots. However, the need of variational solutions (e.g., ONIOM/EE) for a huge number of snapshots makes unpractical the use of state-of-the-art QM Hamiltonians. On the other hand, the effectivity of perturbative approaches (e.g., perturbed matrix method, PMM) comes at the price of poor convergence for configurations strongly different from the reference one. In this paper we introduce an integrated strategy based on a cluster analysis of the MD snapshots. Next, a representative configuration for each cluster is treated at the ONIOM/EE level, whereas local fluctuations within each cluster are described at the PMM level. Some representative systems (uracil in dimethylformamide and in water and tyrosine zwitterion in water) are analyzed to show t..

    Direct Observation of Early-stage Quantum Dot Growth Mechanisms with High-temperature Ab Initio Molecular Dynamics

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    Colloidal quantum dots (QDs) exhibit highly desirable size- and shape-dependent properties for applications from electronic devices to imaging. Indium phosphide QDs have emerged as a primary candidate to replace the more toxic CdSe QDs, but production of InP QDs with the desired properties lags behind other QD materials due to a poor understanding of how to tune the growth process. Using high-temperature ab initio molecular dynamics (AIMD) simulations, we report the first direct observation of the early stage intermediates and subsequent formation of an InP cluster from separated indium and phosphorus precursors. In our simulations, indium agglomeration precedes formation of In-P bonds. We observe a predominantly intercomplex pathway in which In-P bonds form between one set of precursor copies while the carboxylate ligand of a second indium precursor in the agglomerated indium abstracts a ligand from the phosphorus precursor. This process produces an indium-rich cluster with structural properties comparable to those in bulk zinc-blende InP crystals. Minimum energy pathway characterization of the AIMD-sampled reaction events confirms these observations and identifies that In-carboxylate dissociation energetics solely determine the barrier along the In-P bond formation pathway, which is lower for intercomplex (13 kcal/mol) than intracomplex (21 kcal/mol) mechanisms. The phosphorus precursor chemistry, on the other hand, controls the thermodynamics of the reaction. Our observations of the differing roles of precursors in controlling QD formation strongly suggests that the challenges thus far encountered in InP QD synthesis optimization may be attributed to an overlooked need for a cooperative tuning strategy that simultaneously addresses the chemistry of both indium and phosphorus precursors.Comment: 40 pages, 9 figures, submitted for publicatio

    Local Structure in Terms of Nearest-Neighbor Approach in 1-Butyl-3-methylimidazolium-Based Ionic Liquids: MD Simulations

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    Description of the local microscopic structure in ionic liquids (ILs) is a prerequisite to obtain a comprehensive understanding of the influence of the nature of ions on the properties of ILs. The local structure is mainly determined by the spatial arrangement of the nearest neighboring ions. Therefore, the main interaction patterns in ILs, such as cationโ€“anion H-bond-like motifs, cationโ€“cation alkyl tail aggregation, and ring stacking, were considered within the framework of the nearest-neighbor approach with respect to each particular interaction site. We employed classical molecular dynamics (MD) simulations to study in detail the spatial, radial, and orientational relative distribution of ions in a set of imidazolium-based ILs, in which the 1-butyl-3-methylimidazolium (C<sub>4</sub>mim<sup>+</sup>) cation is coupled with the acetate (OAc<sup>โ€“</sup>), chloride (Cl<sup>โ€“</sup>), tetrafluoroborate (BF<sub>4</sub><sup>โ€“</sup>), hexafluorophosphate (PF<sub>6</sub><sup>โ€“</sup>), trifluoromethanesulfonate (TfO<sup>โ€“</sup>), or bisยญ(trifluoromethanesulfonyl)ยญamide (TFSA<sup>โ€“</sup>) anion. It was established that several structural properties are strongly anion-specific, while some can be treated as universally applicable to ILs, regardless of the nature of the anion. Namely, strongly basic anions, such as OAc<sup>โ€“</sup> and Cl<sup>โ€“</sup>, prefer to be located in the imidazolium ring plane next to the Cโ€“H<sup>2/4โ€“5</sup> sites. By contrast, the other four bulky and weakly coordinating anions tend to occupy positions above/below the plane. Similarly, the H-bond-like interactions involving the H<sup>2</sup> site are found to be particularly enhanced in comparison with the ones at H<sup>4โ€“5</sup> in the case of asymmetric and/or more basic anions (C<sub>4</sub>mimOAc, C<sub>4</sub>mimCl, C<sub>4</sub>mimTfO, and C<sub>4</sub>mimTFSA), in accordance with recent spectroscopic and theoretical findings. Other IL-specific details related to the multiple H-bond-like binding and cation stacking issues are also discussed in this paper. The secondary H-bonding of anions with the alkyl hydrogen atoms of cations as well as the cationโ€“cation alkyl chain aggregation turned out to be poorly sensitive to the nature of the anion
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