170 research outputs found

    Diagnosis of Lung Disorder Using Immune Genetic Algorithm and Fuzzy logic to Handle Incertitude

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    In this paper, we present an immune based fuzzy-logic approach for computer-aided diagnosis scheme in medical imaging. The scheme applies to lung CT images and to detect and classify lung nodules. Classification of lung tissue is a significant and challenging task in any computer aided diagnosis system. This paper presents a technique for classification of lung tissue from computed tomography of the lung using the Gaussian interval type-2 fuzzy logic system. The type-2 Gaussian membership functions (T2MFs) and their footprint of uncertainty (FOU) are tuned by immune, genetic algorithm, which is the combination of immune genetic algorithm (GA) and local exploration operator. An immune, genetic algorithm estimates the parameters of the type-2 fuzzy membership function (T2MF). By using immune, genetic algorithm, converging speed is increased. The proposed local exploration operator helps in finding the best Gaussian distribution curve of a particular feature which improves the efficiency and accuracy of the diagnosis system

    An improved data classification framework based on fractional particle swarm optimization

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    Particle Swarm Optimization (PSO) is a population based stochastic optimization technique which consist of particles that move collectively in iterations to search for the most optimum solutions. However, conventional PSO is prone to lack of convergence and even stagnation in complex high dimensional-search problems with multiple local optima. Therefore, this research proposed an improved Mutually-Optimized Fractional PSO (MOFPSO) algorithm based on fractional derivatives and small step lengths to ensure convergence to global optima by supplying a fine balance between exploration and exploitation. The proposed algorithm is tested and verified for optimization performance comparison on ten benchmark functions against six existing established algorithms in terms of Mean of Error and Standard Deviation values. The proposed MOFPSO algorithm demonstrated lowest Mean of Error values during the optimization on all benchmark functions through all 30 runs (Ackley = 0.2, Rosenbrock = 0.2, Bohachevsky = 9.36E-06, Easom = -0.95, Griewank = 0.01, Rastrigin = 2.5E-03, Schaffer = 1.31E-06, Schwefel 1.2 = 3.2E-05, Sphere = 8.36E-03, Step = 0). Furthermore, the proposed MOFPSO algorithm is hybridized with Back-Propagation (BP), Elman Recurrent Neural Networks (RNN) and Levenberg-Marquardt (LM) Artificial Neural Networks (ANNs) to propose an enhanced data classification framework, especially for data classification applications. The proposed classification framework is then evaluated for classification accuracy, computational time and Mean Squared Error on five benchmark datasets against seven existing techniques. It can be concluded from the simulation results that the proposed MOFPSO-ERNN classification algorithm demonstrated good classification performance in terms of classification accuracy (Breast Cancer = 99.01%, EEG = 99.99%, PIMA Indian Diabetes = 99.37%, Iris = 99.6%, Thyroid = 99.88%) as compared to the existing hybrid classification techniques. Hence, the proposed technique can be employed to improve the overall classification accuracy and reduce the computational time in data classification applications

    Image similarity in medical images

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    Image similarity in medical images

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    Recent experiments have indicated a strong influence of the substrate grain orientation on the self-ordering in anodic porous alumina. Anodic porous alumina with straight pore channels grown in a stable, self-ordered manner is formed on (001) oriented Al grain, while disordered porous pattern is formed on (101) oriented Al grain with tilted pore channels growing in an unstable manner. In this work, numerical simulation of the pore growth process is carried out to understand this phenomenon. The rate-determining step of the oxide growth is assumed to be the Cabrera-Mott barrier at the oxide/electrolyte (o/e) interface, while the substrate is assumed to determine the ratio Ξ² between the ionization and oxidation reactions at the metal/oxide (m/o) interface. By numerically solving the electric field inside a growing porous alumina during anodization, the migration rates of the ions and hence the evolution of the o/e and m/o interfaces are computed. The simulated results show that pore growth is more stable when Ξ² is higher. A higher Ξ² corresponds to more Al ionized and migrating away from the m/o interface rather than being oxidized, and hence a higher retained O:Al ratio in the oxide. Experimentally measured oxygen content in the self-ordered porous alumina on (001) Al is indeed found to be about 3% higher than that in the disordered alumina on (101) Al, in agreement with the theoretical prediction. The results, therefore, suggest that ionization on (001) Al substrate is relatively easier than on (101) Al, and this leads to the more stable growth of the pore channels on (001) Al

    μΉ΄μ΄λž„ λ‚˜λ…Έκ΅¬μ‘°μ˜ ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ κΈ°λ°˜ν•œ μ›νŽΈκ΄‘ 이색성 λ³€μ‘°

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    ν•™μœ„λ…Όλ¬Έ(박사) -- μ„œμšΈλŒ€ν•™κ΅λŒ€ν•™μ› : κ³΅κ³ΌλŒ€ν•™ μž¬λ£Œκ³΅ν•™λΆ€, 2022.2. λ‚¨κΈ°νƒœ.μΉ΄μ΄λž„ 메타 λ¬Όμ§ˆμ€ λ›°μ–΄λ‚œ κ΄‘ 물질 μƒν˜Έ μž‘μš©μœΌλ‘œ μΈν•˜μ—¬ λ‚˜λ…Έ κ΄‘μž λΆ„μ•Όμ—μ„œ 큰 관심을 λ°›μ•„μ™”λ‹€. λ‹€λ…„κ°„μ˜ 연ꡬλ₯Ό ν†΅ν•˜μ—¬ μ΅œμ²¨λ‹¨ λ¦¬μ†Œκ·Έλž˜ν”Ό 기술과 λΆ„μž 쑰립 μŠ€μΊν΄λ“œλ₯Ό μ‚¬μš©ν•˜μ—¬ μΉ΄μ΄λž„ λ‚˜λ…Έκ΅¬μ‘°κ°€ μ œμž‘λ˜μ–΄ μ™”λ‹€. κΈ°ν•˜ν•™μ  λΉ„λŒ€μΉ­μ„±μ„ μ§€λ‹ˆλŠ” μΉ΄μ΄λž„ 무기 κΈˆμ† λ‚˜λ…Έ λ¬Όμ§ˆμ€ λŒ€μΉ­μ„±μ„ κ°€μ§€λŠ” λ‚˜λ…Έ λ¬Όμ§ˆμ—μ„œ 얻을 수 μ—†μ—ˆλ˜ λ…νŠΉν•œ 물리적 ν˜„μƒμ„ λ‚˜νƒ€λ‚Ό 수 μžˆλ‹€. μΉ΄μ΄λž„ λ‚˜λ…Έ κ΅¬μ‘°λŠ” 음의 ꡴절λ₯ , λΆ„μž 감지 및 κ΄‘λŒ€μ—­ μ›ν˜• νŽΈκ΄‘κ³Ό 같은 광학적 효과λ₯Ό λ‚˜νƒ€λ‚΄κΈ° μœ„ν•΄ μ‚¬μš©λ  수 μžˆλ‹€. μ΄λŸ¬ν•œ μΉ΄μ΄λž„ 메타 물질의 λ›°μ–΄λ‚œ κ΄‘ν•™ νŠΉμ„±μ„ μ‹€μ œ μž₯μΉ˜μ— ν†΅ν•©ν•˜κΈ° μœ„ν•΄μ„œλŠ” μ„¬μ„Έν•˜κ²Œ μ„€κ³„λœ 광학적 μ„±μ§ˆμ„ κ°€μ§€λŠ” μΉ΄μ΄λž„ ꡬ쑰λ₯Ό λ‹¬μ„±ν•˜λŠ” 것이 ν•„μš”ν•˜λ‹€. κ·ΈλŸ¬λ‚˜ κ³ κ°€μ˜ μ œμ‘°λΉ„μš© 및 μ„€λΉ„, λ³΅μž‘ν•œ 제쑰 κ³Όμ • 및 μ œν•œλœ ν•΄μƒλ„λ‘œ 인해 μΉ΄μ΄λž„ 메타 λ¬Όμ§ˆμ„ μ‹€μ œ μž₯치둜 ν†΅ν•©ν•˜λŠ” 데 μ œν•œμ΄ μžˆμ–΄μ™”λ‹€. μ΄λŸ¬ν•œ ν•œκ³„λ₯Ό κ·Ήλ³΅ν•˜κΈ° μœ„ν•΄μ„œλŠ” μΉ΄μ΄λž„ λ‚˜λ…Έ ꡬ쑰 μ œμ–΄λ₯Ό μœ„ν•œ μœ μ—°ν•œ 방법둠을 κ°œλ°œν•˜λŠ” 것이 μš”κ΅¬λœλ‹€. λ³Έ ν•™μœ„ 연ꡬ μ—μ„œλŠ” νŽ©νƒ€μ΄λ“œλ₯Ό μ΄μš©ν•œ λ‚˜λ…Έ μž…μž ν˜•νƒœμ˜ 닀양화와 λ‚˜λ…Έ κ΅¬μ‘°μ—μ„œμ˜ ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ μ΄μš©ν•œ 광학적 λ°˜μ‘μ˜ 좔가적인 쑰절이 μ•žμ„œ μ–ΈκΈ‰ν•œ ν•œκ³„λ₯Ό ν•΄κ²°ν•˜κΈ° μœ„ν•œ μœ λ§ν•œ λŒ€μ•ˆμ΄ 될 수 μžˆμŒμ„ μ œμ•ˆν•œλ‹€. λ³Έ ν•™μœ„ 논문은 μΉ΄μ΄λž„ λ‚˜λ…Έ ꡬ쑰의 λ°œλ‹¬μ— λŒ€ν•œ 이해와 μ‘°μ ˆμ„ 톡해 ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ μ΄μš©ν•˜μ—¬ μΉ΄μ΄λž„ κ΄‘ν•™ 응닡을 μ‘°μ ˆν•  수 μžˆλŠ” ν”Œλž«νΌμ„ μ œμ‹œν•œλ‹€. μƒμ²΄λΆ„μžλ₯Ό μ΄μš©ν•œ ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ μž…μžμ˜ μ½œλ‘œμ΄λ“œ 합성에 λŒ€ν•œ 졜근 μ—°κ΅¬κ²°κ³ΌλŠ” ν•©μ„± 과정에 κ΄€μ—¬ν•˜λŠ” μΉ΄μ΄λž„μ„± 인코더인 λΆ„μžλ₯Ό λ³€κ²½ν•¨μœΌλ‘œμ¨ μƒˆλ‘œμš΄ ν˜•νƒœμ™€ 광학적 νŠΉμ„±μ„ 가진 λ‚˜λ…Έμž…μžλ₯Ό ν•©μ„±ν•  수 μžˆμŒμ„ μ‹œμ‚¬ν•œλ‹€. λ˜ν•œ 단일 ν”ŒλΌμ¦ˆλͺ¬ μž…μžμ˜ κ΄‘ν•™ 응닡은 ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ μ‚¬μš©ν•˜μ—¬ 증폭되고 λ―Όκ°ν•˜κ²Œ 변쑰될 수 μžˆλ‹€. μ—¬λŸ¬ ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ μž…μžκ°€ 인접할 경우, μž…μž 곡λͺ…μ˜ ν˜Όμ„±ν™”κ°€ μœ λ„λ˜μ–΄ 곡λͺ…을 크게 λ³€ν™”μ‹œν‚¨λ‹€. ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ ꡬ쑰의 ν˜•νƒœμ™€ μΉ΄μ΄λž„μ„±μ„ μ œμ–΄ν•˜κΈ° μœ„ν•œ μƒˆλ‘œμš΄ μ „λž΅μ„ μˆ˜λ¦½ν•˜κΈ° μœ„ν•˜μ—¬, μš°λ¦¬λŠ” λ¨Όμ € μƒμ²΄λΆ„μžμ— μ˜ν•΄ μœ λ„λ˜λŠ” 무기 μΉ΄μ΄λž„μ„±μ— μ΄ˆμ μ„ λ§žμΆ”μ—ˆλ‹€. 무기 ν‘œλ©΄μ—μ„œμ˜ μ›μž μ™œκ³‘ λ˜λŠ” κ±°μ‹œμ  μž¬κ΅¬μ„±μ„ ν†΅ν•œ μΉ΄μ΄λž„μ„±μ˜ 진화에 λŒ€ν•œ κΈ°μ‘΄ μ—°κ΅¬λŠ” μΉ΄μ΄λž„ λ‚˜λ…Έ ꡬ쑰 μ œμ–΄λ₯Ό μœ„ν•œ μƒˆλ‘œμš΄ μ „λž΅ μˆ˜λ¦½μ— μ€‘μš”ν•œ 톡찰λ ₯을 μ œκ³΅ν•œλ‹€. λ³Έ ν•™μœ„λ…Όλ¬Έμ—μ„œλŠ” μΉ΄μ΄λž„ κ΄‘ν•™ λ°˜μ‘μ˜ 이해와 μ‘°μ ˆμ„ 단일 λ‚˜λ…Έ μž…μžμ™€ μ‹œμŠ€ν…œμ  μ œμ–΄μ˜ 두 가지 κ΄€μ μ—μ„œ μ†Œκ°œν•œλ‹€. λ‚˜λ…Έ 재료 κ³΅ν•™μ˜ λ°œμ „μœΌλ‘œ λ‚˜λ…Έ 규λͺ¨μ—μ„œ μ •ν™•ν•œ ν˜•νƒœν•™μ  μ œμ–΄κ°€ κ°€λŠ₯ν•œ μ½œλ‘œμ΄λ“œ ν•©μ„± 방법이 κ°œλ°œλ˜μ—ˆλ‹€. λ‹€μ–‘ν•œ ν• λ‘œκ²ν™”λ¬Ό 이온, κΈˆμ† 이온 및 유기 λΆ„μžλ₯Ό 흑착제둜 μ‚¬μš©ν•˜λ©΄ νŠΉμ • Miller μ§€μˆ˜λ‘œ 결정면을 λΆ€λ™νƒœν™”ν•˜μ—¬ κ²°μ •λ©΄κ³Ό λ‚˜λ…Έμž…μž ν˜•νƒœλ₯Ό μ†μ‰½κ²Œ μ œμ–΄ν•  수 μžˆλ‹€. λ˜ν•œ μ’…μž 맀개 방법은 높은 Miller-index 결정면을 높은 κ· μΌλ„λ‘œ 생성할 수 μžˆμœΌλ―€λ‘œ λ‚˜λ…Έ μž…μžμ˜ ν˜•νƒœλ₯Ό μ œμ–΄ν•˜λŠ” μ€‘μš”ν•œ μ „λž΅μœΌλ‘œ μ‚¬μš©λœλ‹€. μš°λ¦¬λŠ” 합성에 μ²¨κ°€ν•˜λŠ” 유기 λΆ„μžλ₯Ό λ³€κ²½ν•˜μ—¬ 금 λ‚˜λ…Έ μž…μžμ˜ μ„±μž₯ 및 μΉ΄μ΄λž„μ„± 진화에 λŒ€ν•œ κ΄‘λ²”μœ„ν•œ 이해λ₯Ό μ œκ³΅ν•œλ‹€. 이λ₯Ό μœ„ν•˜μ—¬ Ξ³-κΈ€λ£¨νƒ€λ°€μ‹œμŠ€ν…ŒμΈ(Ξ³-Glu-Cys) 및 μ‹œμŠ€ν…Œμ΄λ‹κΈ€λ¦¬μ‹ (Cys-Gly) 을 μ‚¬μš©ν•˜μ—¬ ν•©μ„±λœ 금 λ‚˜λ…Έ μž…μžμ˜ μ„±μž₯ κ²½λ‘œμ™€ ν‚€λž„μ„± 진화가 결정학적 κ΄€μ μ—μ„œ λΆ„μ„λ˜μ—ˆλ‹€. Ξ³-Glu-Cys을 μ΄μš©ν•˜μ—¬ ν•©μ„±λœ 금 λ‚˜λ…Έ μž…μžμ˜ 경우 돌좜된 μΉ΄μ΄λž„ λ‚ κ°œλ₯Ό κ°€μ§€λŠ” μ •μœ‘λ©΄μ²΄ ꡬ쑰둜 λ°œλ‹¬ν•œλ‹€. λ°˜λ©΄μ—, Cys-Gly을 μ΄μš©ν•˜μ—¬ ν•©μ„±λœ λ‚˜λ…Έμž…μžμ˜ 경우 νƒ€μ›ν˜•μ˜ 곡동 ꡬ쑰λ₯Ό 가진 λ§ˆλ¦„λͺ¨κΌ΄ 12면체둜 λ°œλ‹¬ν•˜λ©°, 이둜 인해 두 λ‚˜λ…Έ μž…μžλŠ” μ„œλ‘œ λ‹€λ₯Έ μΉ΄μ΄λž„ κ΄‘ν•™ λ°˜μ‘μ„ 보인닀. μ‹œκ°„μ— λ”°λ₯Έ λ‚˜λ…Έ μž…μžμ˜ μ„±μž₯ 뢄석을 톡해 Ξ³-Glu-Cys와 Cys-Glyκ°€ μ„œλ‘œ λ‹€λ₯Έ 쀑간 ν˜•νƒœλ₯Ό μ§€λ‹ˆλ©° μƒμ„±ν•œλ‹€λŠ” 것을 μ•Œ 수 μžˆμ—ˆλ‹€. Ξ³-Glu-CysλŠ” 였λͺ©ν•œ μœ‘νŒ”λ©΄μ²΄ λͺ¨μ–‘μ˜ 쀑간체λ₯Ό μœ λ„ν•˜λŠ” 반면 Cys-GlyλŠ” 였λͺ©ν•œ λ§ˆλ¦„λͺ¨κΌ΄ μ‹­μ΄λ©΄μ²΄μ˜ 쀑간체λ₯Ό 보인닀. μ΄λŸ¬ν•œ κ²°κ³ΌλŠ” νŽ©νƒ€μ΄λ“œμ™€ 금 ν‘œλ©΄ κ°„μ˜ μƒν˜Έ μž‘μš©μ„ μ΄ν•΄ν•¨μœΌλ‘œμ¨ μΉ΄μ΄λž„ ꡬ쑰와 그에 λ”°λ₯Έ κ΄‘ν•™ λ°˜μ‘μ„ μ‘°μ ˆν•  수 μžˆμŒμ„ μ‹œμ‚¬ν•œλ‹€. 생체 λΆ„μžλ₯Ό μ΄μš©ν•œ μΉ΄μ΄λž„ λ‚˜λ…Έκ΅¬μ‘°μ˜ 합성은 주둜 ν”ŒλΌμ¦ˆλͺ¬ λ¬Όμ§ˆμ—μ„œ μ—°κ΅¬λ˜μ–΄ μ™”μ§€λ§Œ, 촉맀 ν™œμ„±μ„ 지녀 μΉ΄μ΄λž„ μ΄‰λ§€λ‘œ μ‚¬μš©λ  수 μžˆλŠ” μΉ΄μ΄λž„ κΈˆμ† 산화물을 ν•©μ„±ν•˜λ €λŠ” μ‹œλ„ λ˜ν•œ μΉ΄μ΄λž„ 물질의 μ‘μš© ν™•λŒ€λ₯Ό μœ„ν•œ μƒˆλ‘œμš΄ λ°©ν–₯으둜 μ œμ‹œλ˜κ³  μžˆλ‹€. 생체 λΆ„μžλ₯Ό μ΄μš©ν•œ μΉ΄μ΄λž„ κΈˆμ† μ‚°ν™”λ¬Ό ν•©μ„±μ—μ„œμ˜ κΈ°μ‘΄ μ—°κ΅¬λŠ” 단일 아미노산에 κ΅­ν•œλ˜μ–΄ μžˆμ§€λ§Œ, μΉ΄μ΄λž„μ„± λ°œλ‹¬μ„ μ΄ν•΄ν•˜κ³  ν™•μž₯ κ°€λŠ₯ν•œ ν•©μ„± μ „λž΅μ„ μˆ˜λ¦½ν•˜κΈ° μœ„ν•΄μ„œλŠ” νŽ©νƒ€μ΄λ“œλ‘œμ˜ μ„œμ—΄ ν™•μž₯이 μš”κ΅¬λœλ‹€. λ³Έ μ—°κ΅¬μ—μ„œλŠ” Tyr-Tyr-Cys νŽ©νƒ€μ΄λ“œλ₯Ό μ„œμ—΄ν™•μž₯을 μœ„ν•œ λ¦¬κ°„λ“œλ‘œ μ„ νƒν•˜μ—¬, μ½”λ°œνŠΈ μ‚°ν™”λ¬Όμ—μ„œ νŽ©νƒ€μ΄λ“œλ₯Ό μ΄μš©ν•œ μΉ΄μ΄λž„μ„± λ°œν˜„μ„ νƒκ΅¬ν•˜μ˜€λ‹€. νŽ©νƒ€μ΄λ“œ λ¦¬κ°„λ“œλ₯Ό μ΄μš©ν•˜μ—¬ ν•©μ„±λœ μΉ΄μ΄λž„ μ½”λ°œνŠΈ μ‚°ν™”λ¬Ό λ‚˜λ…Έ μž…μžλŠ” μžμ™Έμ„  및 κ°€μ‹œκ΄‘μ„  μ˜μ—­μ—μ„œ 0.01의 λ›°μ–΄λ‚œ λΉ„λŒ€μΉ­ 인자λ₯Ό λ‚˜νƒ€λƒˆλ‹€. λ˜ν•œ, 2D NMR λΆ„κ΄‘ 뢄석을 톡해 λ‚˜λ…Έ μž…μž ν‘œλ©΄μ˜ νŽ©νƒ€μ΄λ“œ λ¦¬κ°„λ“œμ˜ 3차원 μž…μ²΄κ΅¬μ‘°λ₯Ό 규λͺ…ν•˜μ˜€λ‹€. λ˜ν•œ νŽ©νƒ€μ΄λ“œ λ¦¬κ°„λ“œμ˜ μ‹œν€€μŠ€μ— λ”°λ₯Έ μΉ΄μ΄λž„ μ½”λ°œνŠΈ μ‚°ν™”λ¬Ό λ‚˜λ…Έ μž…μžμ˜ λ°œλ‹¬μ„ λΆ„μ„ν•˜μ—¬ Tyr-Tyr-Cys λ¦¬κ°„λ“œμ˜ μ‹Έμ΄μ˜¬ κ·Έλ£Ήκ³Ό 카볡싀 그룹이 μΉ΄μ΄λž„μ„± λ°œλ‹¬μ— μ€‘μš”ν•œ 역할을 담당함을 규λͺ…ν•˜μ˜€λ‹€. λ³Έ 연ꡬ κ²°κ³ΌλŠ” 무기 결정에 μΉ΄μ΄λž„μ„±μ„ λ°œν˜„ν•˜λŠ” νŽ©νƒ€μ΄λ“œμ˜ 역할이 μƒν˜Έ μž‘μš©ν•˜λŠ” λ¬Όμ§ˆμ— 따라 λ‹¬λΌμ§ˆ 수 있으며, μΉ΄μ΄λž„ κ΄‘ν•™ νŠΉμ„±μ˜ λ³€ν™”λ₯Ό μ•ΌκΈ°ν•  수 μžˆμŒμ„ μ‹œμ‚¬ν•œλ‹€. 단일 ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ μž…μžμ˜ κ΄‘ν•™ μ‹ ν˜ΈλŠ” ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ ν†΅ν•˜μ—¬ 증폭되고 λ―Όκ°ν•˜κ²Œ μ œμ–΄λ  수 μžˆλ‹€. μ—¬λŸ¬ 개의 ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ μž…μžκ°€ 인접할 경우, μž…μž 곡λͺ…μ˜ ν˜Όμ„±ν™”κ°€ μΌμ–΄λ‚˜ 곡λͺ…을 크게 λ³€ν™”μ‹œν‚¨λ‹€. μ΄λŸ¬ν•œ λ§₯λ½μ—μ„œ, λ³Έ μ—°κ΅¬μ—μ„œλŠ” ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ μΉ΄μ΄λž„ ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έ μž…μžμ— μ μš©ν•˜μ—¬ μΉ΄μ΄λž„ κ΄‘ν•™ νŠΉμ„±μ„ μ œμ–΄ν•˜κ³ μž ν•˜μ˜€λ‹€. 이λ₯Ό μœ„ν•˜μ—¬ μΉ΄μ΄λž„ 금 λ‚˜λ…Έ μž…μžλ₯Ό κΈ°νŒμ— μ½”νŒ…ν•˜κ³  λ‚˜λ…Έ 크기의 ν”ŒλΌμ¦ˆλͺ¬ κΈˆμ† 측을 μ¦μ°©ν•˜μ—¬ 메타 λ¬Όμ§ˆμ„ μ œμž‘ν•˜μ˜€λ‹€. ν”ŒλΌμ¦ˆλͺ¬ κ²°ν•©μœΌλ‘œ μΈν•œ κ΄‘ν•™ νŠΉμ„±μ˜ λ³€ν™”λŠ” 투과 기반 및 ν™•μ‚° λ°˜μ‚¬ 기반 μ›νŽΈκ΄‘ 이색성 (cirular dichroism, CD) 뢄광법을 톡해 λΆ„μ„λ˜μ—ˆλ‹€. μΉ΄μ΄λž„ κΈˆμ† λ‚˜λ…Έ μž…μž 기반 메타 물질의 광학적 뢄석을 톡해 CD μŠ€νŽ™νŠΈλŸΌμ˜ 피크 μœ„μΉ˜, μ„ΈκΈ° 및 λΆ€ν˜Έκ°€ ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ— μ˜ν•΄ 변화함을 μ•Œ 수 μžˆμ—ˆλ‹€. λ˜ν•œ, ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ— μ˜ν•΄ μƒμ„±λœ λͺ¨λ“œλŠ” λ‚˜λ…Έκ΅¬μ‘°μ²΄μ˜ 크기, 거리 및 μ£Όλ³€ ꡴절λ₯ μ— 따라 크게 λ³€ν™”ν•˜μ˜€λ‹€. 더 λ‚˜μ•„κ°€, μΉ΄μ΄λž„ 금 λ‚˜λ…Έ μž…μžμ— 싀리카 μ‰˜μ˜ ν”ŒλΌμ¦ˆλͺ¬ λ‚˜λ…Έμž…μžμ˜ κ΄‘ν•™ νŠΉμ„± 및 μ•ˆμ •μ„±μ˜ μ œμ–΄κ°€ κ°€λŠ₯함을 규λͺ…ν•˜μ˜€λ‹€. λ³Έ ν•™μœ„ μ—°κ΅¬μ—μ„œλŠ” λ‚˜λ…Έ μž…μžμ˜ μΉ΄μ΄λž„μ„± λ°œλ‹¬μ— νŽ©νƒ€μ΄λ“œ λ¦¬κ°„λ“œκ°€ λ―ΈμΉ˜λŠ” 역할을 μ΄ν•΄ν•¨μœΌλ‘œμ¨ 단일 λ‚˜λ…Έ μž…μž μˆ˜μ€€μ—μ„œ CD μ‹ ν˜Έμ˜ μ œμ–΄λ₯Ό λ‹¬μ„±ν•˜μ˜€λ‹€. λ˜ν•œ ν”ŒλΌμ¦ˆλͺ¬ μ»€ν”Œλ§μ„ μ‚¬μš©ν•˜μ—¬ μΉ΄μ΄λž„ λ‚˜λ…Έ ꡬ쑰의 광학적 νŠΉμ„±μ„ μ‘°μ ˆν•˜λŠ” 방법둠이 ν™•λ¦½λ˜μ—ˆλ‹€. λ³Έ 연ꡬλ₯Ό ν†΅ν•˜μ—¬ 개발된 μΉ΄μ΄λž„ λ‚˜λ…Έ κ΅¬μ‘°μ—μ„œ κ΄‘ν•™ νŠΉμ„±μ˜ μ‘°μ ˆμ„ μœ„ν•œ 방법둠은 μΉ΄μ΄λž„ 메타 λ¬Όμ§ˆμ„ μ‹€μš©μ μΈ κ΄‘ν•™ μž₯치둜 ν†΅ν•©ν•˜λŠ” 것을 μš©μ΄ν•˜κ²Œ ν•  κ²ƒμœΌλ‘œ κΈ°λŒ€λœλ‹€.Chiral metamaterials have been actively pursued in the field of nanophotonics due to their exceptional light-matter interactions. For decades, numerous attempts have been conducted to fabricate chiral nanostructure using state-of-the-art lithography techniques and molecular-assembly scaffolds. Possessing this geometric property, inorganic metal nanomaterials could exhibit fascinating physical phenomena which was difficult to be achieved in symmetric nanomaterials. Chiral nanostructures have greatly expanded the design to demonstrate chiroptic effects such as a negative refractive index, sensitive chiral sensing, and broad-band circular polarizer. In order to integrate the fascinating properties of chiral metamaterials into practical devices, it is necessary to achieve precisely defined chiral morphologies and chiroptic properties. However, the requirement for expensive facilities, the complexity of the process, and the limited resolution had restricted the translation of chiral metamaterials into real devices. Therefore, developing flexible methodologies for nanostructure control is important to address these limitations and provide new directions. Through this study, we propose that the diversification of nanoparticle morphology using peptide molecules and further modulation of the optical response utilizing plasmonic coupling of nanostructures can be a promising alternative to solve the above-mentioned limitations. In this thesis, we present a platform that can modulate the chiroptic response using plasmon coupling through understanding and regulation of the development of chiral nanostructures. Recent study on the colloidal synthesis of plasmonic nanoparticles using biomolecules suggests that nanoparticles with novel morphology and optical property can be achieved by altering molecules, which are chirality encoders, involved during the synthesis. In addition, the optical response of a single plasmonic particle can be amplified and sensitively modulated using plasmon coupling. When several nanoscale plasmonic particles are adjacent to each other, hybridization of particle resonance is induced, which significantly changes the resonance. To establish new strategies for controlling the morphology and chirality of plasmonic nanostructures, we have first studied previous studies on bio-inspired pathways for complex nanostructures, focusing on the inorganic chirality induced by biomolecules in Chapter 2. Importantly, the interactions at the interface between biomolecules and inorganic surfaces provide an important insight into the evolution of chirality through atomic distortion or macroscopic reconstruction. Chapter 3 describes the experimental procedures, and Chapter 4, 5, and 6 describe the understanding and modulation of the chiroptic response from the two perspectives of single nanoparticles and systemic control. Advances in nanomaterial engineering have enabled the development of colloidal synthesis methods for precise morphological control at the nanoscale. The use of various halide ions, metal ions and organic molecules as adsorbates can control the crystal facet and nanoparticle morphology by passivating the crystal facet with a specific Miller index. In addition, the seed-mediated method can synthesize high-Miller-index crystal facets with high uniformity, and thus is being used as an important strategy for controlling NP morphology. In this thesis, we have provided a broad understanding of the growth and chirality evolution in gold NPs by adjusting the type of additive molecules. We have analyzed the growth pathway and chirality evolution of the Ξ³-glutamylcysteine- (Ξ³-Glu-Cys-) and cysteinylglycine- (Cys-Gly-) directed gold NPs from a crystallographic perspective. Gold NPs developed into a cube-like structure with protruding chiral wings in the presence of Ξ³-Glu-Cys, whereas the NPs synthesized with Cys-Gly exhibited a rhombic dodecahedron-like outline with elliptical cavity structures, showing different chiroptic responses. Through time-dependent analysis, we reported that Ξ³-Glu-Cys and Cys-Gly generate different intermediate morphologies. Ξ³-Glu-Cys induced concave hexoctahedra-shaped intermediate, whereas Cys-Gly showed concave rhombic dodecahedra-shaped intermediate. These results showed that the chiral structure and resulting chiroptic response can be modulated through understanding the interaction between peptides and gold surfaces. Molecule-directed synthesis of chiral nanostructure has been mainly studied in plasmonic materials, but attempts to synthesize chiral metal oxides that can be used as chiral catalysts due to their catalytic activity has been suggested as a new direction for expanding the application of chiral materials. Existing studies on the synthesis of chiral metal oxide using molecule have been limited to single amino acids, but sequence expansion with peptides is required to understand the chirality evolution and achieve a scalable synthetic strategy. In this thesis, Tyr-Tyr-Cys tripeptide including tyrosine and cysteine were selected as peptide ligands and the role of peptide in developing chirality in cobalt oxide was explored. Synthesized chiral cobalt oxide nanoparticles showed a g-factor of 0.01 in the UV–visible region. In addition, the 3D conformation of the peptide ligand on the nanoparticle surfaces was identified by 2D NMR spectroscopy analysis. Furthermore, the sequence effect of Tyr-Tyr-Cys developing chiral cobalt oxide was analyzed, demonstrating that the thiol group and carboxyl group of the Tyr-Tyr-Cys ligand played an important role in chirality evolution. This results suggest that the role of the peptides can vary depending on the interacting material, leading to further variability in chiroptical properties. The optical signal of a single plasmonic particle can be amplified and sensitively controlled using plasmon coupling. When several nanoscale plasmonic particles are adjacent to each other, hybridization of particle resonance occurs, which significantly changes the resonance. In this context, plasmonic coupling which has been mainly studied in achiral plasmon structures, was applied to chiral plasmonic nanoparticles to control chiroptical properties. In this thesis, we demonstrated the fabrication of metamaterial by coating chiral gold nanoparticles on a substrate and depositing a nanoscale plasmonic metal layer. In order to investigate changes in optical properties due to plasmon coupling, transmission-based and diffuse reflectance circular dichroism (CD) spectroscopy were utilized. Through this, it was confirmed that the resonance position, magnitude, and sign of the CD spectrum were changed by plasmon coupling. In addition, the coupled plasmon mode was significantly changed according to the dimension, distance, and refractive index of the nanostructure. Furthermore, synthesis of chiral gold-silica core-shell NPs enables versatile control of the structure and properties of plasmonic nanoparticles, facilitating their application to tailored plasmon coupling. In conclusion, by understanding the role of peptides in nanoparticle development, CD manipulation has been achieved at the single nanoparticle level. In addition, a methodology for modulating the optical properties of chiral nanostructures using plasmon coupling has been established. We believe the development of versatile methodology for modulation of the chiroptical response in chiral nanostructures ultimately facilitate integration of the chiral metamaterials into practical optical devices.Chapter 1. Introduction 1 1.1 Chirality in Nature 1 1.2 Chiral Plasmonic Nanostructure 9 1.3 Objective of Thesis 21 Chapter 2. Fabrication of Chiral Inorganic Nanostructure and Its Optical Properties 24 2.1 Fabrication of Chiral Nanostructures using Hard Approach 24 2.2 Biomolecule-Directed Chiral Nanostructure 29 2.2.1 Biomolecule-Conjugated Inorganic Nanoparticles 29 2.2.2 Chirality Development by Biomolecule-Induced Local Distortion 36 2.2.3 Biomolecule-Directed Chiral Morphology 44 Chapter 3. Experimental Procedures 62 3.1 Synthesis of Chiral Gold Nanoparticles 62 3.2 Synthesis of Chiral Cobalt Oxide Nanoparticles 64 3.3 Synthesis of Chiral Gold-Silica Core-Shell Nanoparticles 66 3.4 Optical Characterization of Chiral Nanostructures 67 Chapter 4. Dipeptide-Directed Chiral Gold Nanoparticles 69 4.1 Introduction 69 4.2 Solution-Based Synthesis of Dipeptide-Directed Chiral NPs 72 4.3 Morphology Analysis of Ξ³-Glu-Cys- and Cys-Gly-directed NPs 79 4.4 Time-Dependent Analysis of Chiral Morphology Development 83 4.5 Concentration-Dependent Chiral Morphology and Chiroptical Responses 91 4.6 Sequence Effects 101 4.7 Conclusion 102 Chapter 5. Peptide-Directed Chiral Cobalt Oxide Nanoparticle 103 5.1 Introduction 103 5.2 Synthesis of Chiral Cobalt Oxide Nanoparticles using Tyr-Tyr-Cys 107 5.3 Effect of Synthetic Parameters on Chirality Development of Chiral Cobalt Oxide Nanoparticles 114 5.4 3D Conformation of Tyr-Tyr-Cys Ligand 120 5.5 Sequence Effect of the Tyr-Tyr-Cys 125 5.6 Magnetic Circular Dichroism in Chiral Cobalt Oxide Nanoparticles. 129 5.7 Conclusion 134 Chapter 6. Circular Dichroism Manipulation based on Plasmonic Coupling of Chiral Nanostructures 136 6.1 Introduction 136 6.2 Chiroptical Property of Helicoid-Based Plasmonic Nanostructure 138 6.3 Effect of Chiral Gap Structure 145 6.4 Spectral Manipulation through Structural Parameter Control 149 6.5 Synthesis of Chiral Gold-Silica Core-Shell Nanoparticles 151 6.6 Conclusion 154 Chapter 7. Concluding Remarks 155 References 159λ°•

    Innovative techniques to devise 3D-printed anatomical brain phantoms for morpho-functional medical imaging

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    Introduction. The Ph.D. thesis addresses the development of innovative techniques to create 3D-printed anatomical brain phantoms, which can be used for quantitative technical assessments on morpho-functional imaging devices, providing simulation accuracy not obtainable with currently available phantoms. 3D printing (3DP) technology is paving the way for advanced anatomical modelling in biomedical applications. Despite the potential already expressed by 3DP in this field, it is still little used for the realization of anthropomorphic phantoms of human organs with complex internal structures. Making an anthropomorphic phantom is very different from making a simple anatomical model and 3DP is still far from being plug-and-print. Hence, the need to develop ad-hoc techniques providing innovative solutions for the realization of anatomical phantoms with unique characteristics, and greater ease-of-use. Aim. The thesis explores the entire workflow (brain MRI images segmentation, 3D modelling and materialization) developed to prototype a new complex anthropomorphic brain phantom, which can simulate three brain compartments simultaneously: grey matter (GM), white matter (WM) and striatum (caudate nucleus and putamen, known to show a high uptake in nuclear medicine studies). The three separate chambers of the phantom will be filled with tissue-appropriate solutions characterized by different concentrations of radioisotope for PET/SPECT, para-/ferro-magnetic metals for MRI, and iodine for CT imaging. Methods. First, to design a 3D model of the brain phantom, it is necessary to segment MRI images and to extract an error-less STL (Standard Tessellation Language) description. Then, it is possible to materialize the prototype and test its functionality. - Image segmentation. Segmentation is one of the most critical steps in modelling. To this end, after demonstrating the proof-of-concept, a multi-parametric segmentation approach based on brain relaxometry was proposed. It includes a pre-processing step to estimate relaxation parameter maps (R1 = longitudinal relaxation rate, R2 = transverse relaxation rate, PD = proton density) from the signal intensities provided by MRI sequences of routine clinical protocols (3D-GrE T1-weighted, FLAIR and fast-T2-weighted sequences with ≀ 3 mm slice thickness). In the past, maps of R1, R2, and PD were obtained from Conventional Spin Echo (CSE) sequences, which are no longer suitable for clinical practice due to long acquisition times. Rehabilitating the multi-parametric segmentation based on relaxometry, the estimation of pseudo-relaxation maps allowed developing an innovative method for the simultaneous automatic segmentation of most of the brain structures (GM, WM, cerebrospinal fluid, thalamus, caudate nucleus, putamen, pallidus, nigra, red nucleus and dentate). This method allows the segmentation of higher resolution brain images for future brain phantom enhancements. - STL extraction. After segmentation, the 3D model of phantom is described in STL format, which represents the shapes through the approximation in manifold mesh (i.e., collection of triangles, which is continuous, without holes and with a positive – not zero – volume). For this purpose, we developed an automatic procedure to extract a single voxelized surface, tracing the anatomical interface between the phantom's compartments directly on the segmented images. Two tubes were designed for each compartment (one for filling and the other to facilitate the escape of air). The procedure automatically checks the continuity of the surface, ensuring that the 3D model could be exported in STL format, without errors, using a common image-to-STL conversion software. Threaded junctions were added to the phantom (for the hermetic closure) using a mesh processing software. The phantom's 3D model resulted correct and ready for 3DP. Prototyping. Finally, the most suitable 3DP technology is identified for the materialization. We investigated the material extrusion technology, named Fused Deposition Modeling (FDM), and the material jetting technology, named PolyJet. FDM resulted the best candidate for our purposes. It allowed materializing the phantom's hollow compartments in a single print, without having to print them in several parts to be reassembled later. FDM soluble internal support structures were completely removable after the materialization, unlike PolyJet supports. A critical aspect, which required a considerable effort to optimize the printing parameters, was the submillimetre thickness of the phantom walls, necessary to avoid distorting the imaging simulation. However, 3D printer manufacturers recommend maintaining a uniform wall thickness of at least 1 mm. The optimization of printing path made it possible to obtain strong, but not completely waterproof walls, approximately 0.5 mm thick. A sophisticated technique, based on the use of a polyvinyl-acetate solution, was developed to waterproof the internal and external phantom walls (necessary requirement for filling). A filling system was also designed to minimize the residual air bubbles, which could result in unwanted hypo-intensity (dark) areas in phantom-based imaging simulation. Discussions and conclusions. The phantom prototype was scanned trough CT and PET/CT to evaluate the realism of the brain simulation. None of the state-of-the-art brain phantoms allow such anatomical rendering of three brain compartments. Some represent only GM and WM, others only the striatum. Moreover, they typically have a poor anatomical yield, showing a reduced depth of the sulci and a not very faithful reproduction of the cerebral convolutions. The ability to simulate the three brain compartments simultaneously with greater accuracy, as well as the possibility of carrying out multimodality studies (PET/CT, PET/MRI), which represent the frontier of diagnostic imaging, give this device cutting-edge prospective characteristics. The effort to further customize 3DP technology for these applications is expected to increase significantly in the coming years

    Air Force Institute of Technology Research Report 2020

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    This Research Report presents the FY20 research statistics and contributions of the Graduate School of Engineering and Management (EN) at AFIT. AFIT research interests and faculty expertise cover a broad spectrum of technical areas related to USAF needs, as reflected by the range of topics addressed in the faculty and student publications listed in this report. In most cases, the research work reported herein is directly sponsored by one or more USAF or DOD agencies. AFIT welcomes the opportunity to conduct research on additional topics of interest to the USAF, DOD, and other federal organizations when adequate manpower and financial resources are available and/or provided by a sponsor. In addition, AFIT provides research collaboration and technology transfer benefits to the public through Cooperative Research and Development Agreements (CRADAs). Interested individuals may discuss ideas for new research collaborations, potential CRADAs, or research proposals with individual faculty using the contact information in this document
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