629 research outputs found

    Inventing episodic memory : a theory of dorsal and ventral hippocampus

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    Contention resolution in optical packet-switched cross-connects

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    Magnetoencephalography

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    This is a practical book on MEG that covers a wide range of topics. The book begins with a series of reviews on the use of MEG for clinical applications, the study of cognitive functions in various diseases, and one chapter focusing specifically on studies of memory with MEG. There are sections with chapters that describe source localization issues, the use of beamformers and dipole source methods, as well as phase-based analyses, and a step-by-step guide to using dipoles for epilepsy spike analyses. The book ends with a section describing new innovations in MEG systems, namely an on-line real-time MEG data acquisition system, novel applications for MEG research, and a proposal for a helium re-circulation system. With such breadth of topics, there will be a chapter that is of interest to every MEG researcher or clinician

    Developing structured representations

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    Laser-induced forward transfer (LIFT) of water soluble polyvinyl alcohol (PVA) polymers for use as support material for 3D-printed structures

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    The additive microfabrication method of laser-induced forward transfer (LIFT) permits the creation of functional microstructures with feature sizes down to below a micrometre [1]. Compared to other additive manufacturing techniques, LIFT can be used to deposit a broad range of materials in a contactless fashion. LIFT features the possibility of building out of plane features, but is currently limited to 2D or 2ยฝD structures [2โ€“4]. That is because printing of 3D structures requires sophisticated printing strategies, such as mechanical support structures and post-processing, as the material to be printed is in the liquid phase. Therefore, we propose the use of water-soluble materials as a support (and sacrificial) material, which can be easily removed after printing, by submerging the printed structure in water, without exposing the sample to more aggressive solvents or sintering treatments. Here, we present studies on LIFT printing of polyvinyl alcohol (PVA) polymer thin films via a picosecond pulsed laser source. Glass carriers are coated with a solution of PVA (donor) and brought into proximity to a receiver substrate (glass, silicon) once dried. Focussing of a laser pulse with a beam radius of 2 ยตm at the interface of carrier and donor leads to the ejection of a small volume of PVA that is being deposited on a receiver substrate. The effect of laser pulse fluence , donor film thickness and receiver material on the morphology (shape and size) of the deposits are studied. Adhesion of the deposits on the receiver is verified via deposition on various receiver materials and via a tape test. The solubility of PVA after laser irradiation is confirmed via dissolution in de-ionised water. In our study, the feasibility of the concept of printing PVA with the help of LIFT is demonstrated. The transfer process maintains the ability of water solubility of the deposits allowing the use as support material in LIFT printing of complex 3D structures. Future studies will investigate the compatibility (i.e. adhesion) of PVA with relevant donor materials, such as metals and functional polymers. References: [1] A. Piquรฉ and P. Serra (2018) Laser Printing of Functional Materials. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA. [2] R. C. Y. Auyeung, H. Kim, A. J. Birnbaum, M. Zalalutdinov, S. A. Mathews, and A. Piquรฉ (2009) Laser decal transfer of freestanding microcantilevers and microbridges, Appl. Phys. A, vol. 97, no. 3, pp. 513โ€“519. [3] C. W. Visser, R. Pohl, C. Sun, G.-W. Rรถmer, B. Huis in โ€˜t Veld, and D. Lohse (2015) Toward 3D Printing of Pure Metals by Laser-Induced Forward Transfer, Adv. Mater., vol. 27, no. 27, pp. 4087โ€“4092. [4] J. Luo et al. (2017) Printing Functional 3D Microdevices by Laser-Induced Forward Transfer, Small, vol. 13, no. 9, p. 1602553

    ๊ณ ์ถœ๋ ฅ ์–‘์„ฑ์ž ์ž…์‚ฌ๊ธฐ์—์„œ ์ €์—๋„ˆ์ง€ ๋น” ์ˆ˜์†ก ํ–ฅ์ƒ์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์—๋„ˆ์ง€์‹œ์Šคํ…œ๊ณตํ•™๋ถ€, 2021.8. ๊น€๋™ํ™˜.A proton injector is the key element of a high current beam and high-performance fast neutron sources for basic science and future energy resources. The proton injector in the study transports a high-current and low-energy proton beam with minimum loss and makes the beam parameters matched to a subsequent accelerator such as radio-frequency quadrupole. A high-current proton beam contains strong space charge effect and non-linear electric field, increasing beam size and emittance during transport. To reduce the beam size, solenoid focusing lens is used, which rather causes spherical aberration and another emittance growth. In addition, the presence of such an electromagnetic element gives rise to alignment error. Solenoid magnet makes it difficult to control a position of beam centroid since it has characteristics of rotating and coupling the beam in the transverse plane. This study has established a proton injector test stand and introduced novel techniques to improve the low energy beam transport in a high-intensity proton injector. Proton injector test stand includes transverse beam profile monitor, which is composed of a scintillation screen and a CCD camera, to measure the position, size, and emittance of the beam. Two key factors for improving low-energy beam transport are low beam emittance and a fast and accurate beam tuning method. For this purpose, a residual gas molecule analysis method and an artificial neural network (ANN) model are introduced. As a first result, low beam emittance was measured by preventing beam emittance from growing through an inert gas injection technique based on numerical analysis on steady-state pressure in high vacuum condition. A space charge potential increases beam emittance, not preserving the intrinsic emittance at the beam extraction region. One of the natural processes to cancel space charge force is that proton beam collides with residual gases mainly composed of hydrogen molecules flowing out of ion source and air molecules, causing some ionization. It is a self-neutralization that the generated electrons are trapped in the space charge potential of the beam. It is known to be more effective as the number of residual gas molecules in the transport pipe increases and the heavier inert gas molecules are involved since they generally have larger collisional cross-section. Suppression of emittance growth is achieved and beam emittance is decreased up to 23% through the residual gas injection. Artificial neural network (ANN) model can greatly reduce time and increase accuracy in low energy beam tuning. There are unknowns such as alignment errors that are difficult to measure between elements involved in the beam transport process, such as beam extraction, focusing, and deflection. To correct for these errors, steering magnets control the beam centroid in the transverse plane. In order to optimize the beam transport, it is necessary to observe the change of beam centroid and size for various magnet settings. Multi-layer perceptron model is utilized to interpret this nonlinear relationship and to control the beam properly based on the measured data. Extensive beam dynamics simulations are performed to verify the efficient training and the practicality of the predictive model. The output results of calculating the beam size and beam position at a specific location are obtained according to various sources of errors and unknowns that may occur in the LEBT. It is confirmed that the predictive model with high accuracy can be derived from sufficient measurement data, and it is applied to actual beam diagnosis and beam control experiments. The ANN model developed in this study shows more accurate prediction at a speed 49 times faster than the existing scan method. This study contributed to the suppression of the beam emittance growth and the development of a fast and accurate beam transport control technique in high intensity proton injector. This can be applied to the evaluation and improvement of beam emittance in beamlines under various conditions by increasing the utility of beam diagnostic data. In addition, there is a possibility to greatly improve beam tuning efficiency to higher energy sections and beamlines that have more control variables and are more complex than low-energy beam transport systems. Ultimately, the study can be developed as a base technology for autonomous operation of accelerator with minimum human intervention.๊ณ ์ถœ๋ ฅ ์–‘์„ฑ์ž ๊ฐ€์†๊ธฐ๋Š” ์ž˜ ์ •๋ฆฝ๋œ ๊ธฐ์ˆ ๊ณผ ์—ฐ์† ์šด์ „์„ฑ์„ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•˜์—ฌ ๊ณ ์„ฑ๋Šฅ ๊ณ ์† ์ค‘์„ฑ์ž์› ๊ฐœ๋ฐœ์— ์ฃผ๋กœ ์‘์šฉ๋œ๋‹ค. ๊ทธ ์ค‘์—์„œ ์–‘์„ฑ์ž ์ž…์‚ฌ๊ธฐ๋Š” ๋†’์€ ์ „๋ฅ˜์˜ ๋น”์„ ์–ป๊ธฐ ์œ„ํ•œ ์ค‘์š”ํ•œ ๊ธฐ๋ฐ˜์ด๋‹ค. ์ด ์žฅ์น˜๋Š” ์ด์˜จ์›์—์„œ ํ˜•์„ฑ๋œ ์ดˆ๊ธฐ ๋น”์„ ์ตœ์†Œํ•œ์˜ ์†์‹ค๋กœ ์ˆ˜์†กํ•˜๊ณ , ๊ณ ์ฃผํŒŒ ์‚ฌ์ค‘๊ทน๊ณผ ๊ฐ™์€ ํ›„์† ๊ฐ€์†๊ด€์ด ์š”๊ตฌํ•˜๋Š” ์ž…๋ ฅ ๋น” ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ์ •ํ•ฉ์‹œํ‚ค๋Š” ์—ญํ• ์„ ์ˆ˜ํ–‰ํ•œ๋‹ค. ๊ณ ์ „๋ฅ˜ ๋น”์€ ๋น„์„ ํ˜•์ ์ธ ์ „๊ธฐ์žฅ ์„ฑ๋ถ„์„ ํฌํ•จํ•˜์—ฌ ๊ฐ•ํ•œ ๊ณต๊ฐ„ ์ „ํ•˜ ํšจ๊ณผ๋ฅผ ์ผ์œผํ‚ค๊ธฐ ๋•Œ๋ฌธ์—, ์ˆ˜์†ก ๊ณผ์ •์—์„œ ๋น” ํฌ๊ธฐ์™€ ์—๋ฏธํ„ด์Šค๊ฐ€ ์ƒ์Šนํ•˜๋Š” ๋ฌธ์ œ๊ฐ€ ์žˆ๋‹ค. ๋น” ํฌ๊ธฐ๋ฅผ ์ค„์ด๊ธฐ ์œ„ํ•ด ์†”๋ ˆ๋…ธ์ด๋“œ ์ง‘์† ๋ Œ์ฆˆ๋ฅผ ์ด์šฉํ•˜๋Š”๋ฐ, ์ด๋Š” ์˜คํžˆ๋ ค ๊ตฌ๋ฉด ์ˆ˜์ฐจ๋ฅผ ์ผ์œผํ‚ค๋ฉฐ ์—๋ฏธํ„ด์Šค๋ฅผ ๋ณด์กด์‹œํ‚ค์ง€ ๋ชปํ•œ๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ „์ž์„๊ณผ ๊ฐ™์€ ๋น” ์ˆ˜์†ก ์š”์†Œ๋Š” ์ˆ˜์†ก๊ด€์˜ ์ •๋ ฌ ์˜ค์ฐจ๋ฅผ ์ผ์œผํ‚จ๋‹ค. ํŠนํžˆ, ์†”๋ ˆ๋…ธ์ด๋“œ ์ „์ž์„์€ ๋น”์„ ํšก๋ฐฉํ–ฅ์œผ๋กœ ํšŒ์ „์‹œํ‚ค๋Š” ํŠน์„ฑ์ด ์žˆ๊ธฐ ๋•Œ๋ฌธ์— ์ •๋ ฌ ์˜ค์ฐจ์™€ ๋”๋ถˆ์–ด ๋น” ์ค‘์‹ฌ ์œ„์น˜ ์ œ์–ด๋ฅผ ๋”์šฑ ์–ด๋ ต๊ฒŒ ๋งŒ๋“ ๋‹ค. ์ด ์—ฐ๊ตฌ๋Š” ๊ณ ์ถœ๋ ฅ ์–‘์„ฑ์ž ์ž…์‚ฌ๊ธฐ์˜ ์ €์—๋„ˆ์ง€ ๋น” ์ˆ˜์†ก ์„ฑ๋Šฅ ํ–ฅ์ƒ์„ ์œ„ํ•œ ๊ธฐ๋ฒ• ๊ฐœ๋ฐœ์„ ๋ชฉํ‘œ๋กœ ํ•˜๊ณ , ์ž…์‚ฌ๊ธฐ ์‹œํ—˜ ์‹œ์„ค์„ ๊ตฌ์ถ•ํ•œ๋‹ค. ์„ฑ๋Šฅ ๊ฐœ์„ ์„ ์‹คํ—˜์ ์œผ๋กœ ํ™•์ธํ•˜๊ธฐ ์œ„ํ•ด ์„ฌ๊ด‘ํŒ๊ณผ CCD ์นด๋ฉ”๋ผ๋ฅผ ์ด์šฉํ•œ ๋น” ํ”„๋กœํŒŒ์ผ ๋ชจ๋‹ˆํ„ฐ๋ฅผ ์ฃผ์š” ์ง„๋‹จ ์žฅ์น˜๋กœ ์ด์šฉํ•œ๋‹ค. ์ €์—๋„ˆ์ง€ ๋น” ์ˆ˜์†ก ์„ฑ๋Šฅ์˜ ํ•ต์‹ฌ ์š”์†Œ ๋‘ ๊ฐ€์ง€๋Š” ๋‚ฎ์€ ๋น” ์—๋ฏธํ„ด์Šค์™€ ๋น ๋ฅด๊ณ  ์ •ํ™•ํ•œ ๋น” ํŠœ๋‹ ๋ฐฉ๋ฒ•์ด๋‹ค. ์ด๋ฅผ ์œ„ํ•ด ์ž”๋ฅ˜ ๋ถ„์ž ํ•ด์„ ๋ฐฉ๋ฒ•๊ณผ ๊ธฐ๊ณ„ ํ•™์Šต ๊ธฐ๋ฒ•์„ ๊ฐ๊ฐ ๋„์ž…ํ•œ๋‹ค. ์ฒซ ๋ฒˆ์งธ ๊ฒฐ๊ณผ๋กœ, ์ž”๋ฅ˜ ๋ถ„์ž ํ•ด์„์„ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•œ ๋น„ํ™œ์„ฑ ๊ธฐ์ฒด ์ฃผ์ž… ๊ธฐ๋ฒ•์„ ํ†ตํ•ด ๋น” ์—๋ฏธํ„ด์Šค ์„ฑ์žฅ์„ ๋ง‰์•„ ๋‚ฎ์€ ๋น” ์—๋ฏธํ„ด์Šค๋ฅผ ์ธก์ •ํ•œ๋‹ค. ๊ณ ์ „๋ฅ˜ ๋น”์˜ ๋†’์€ ๊ณต๊ฐ„ ์ „ํ•˜ ํฌํ…์…œ์€ ๋น”์ด ์ง„ํ–‰ํ•จ์— ๋”ฐ๋ผ ๋น” ์—๋ฏธํ„ด์Šค๋ฅผ ์ƒ์Šน์‹œํ‚ค๋Š” ๋ฌธ์ œ๊ฐ€ ์žˆ๋‹ค. ์ด๋ฅผ ์ƒ์‡„์‹œํ‚ค๋Š” ์ž์—ฐ์Šค๋Ÿฌ์šด ๊ณผ์ • ์ค‘ ํ•˜๋‚˜๋Š”, ์–‘์„ฑ์ž ์ž…์‚ฌ๊ธฐ์˜ ๊ฒฝ์šฐ ์ˆ˜์†Œ ์ด์˜จ์›์—์„œ ํ˜๋Ÿฌ๋‚˜์˜จ ์ˆ˜์†Œ ๋ถ„์ž์™€, ๋ฏธ๋Ÿ‰์œผ๋กœ ์œ ์ž…๋˜์–ด ํ‰ํ˜•์„ ์ด๋ฃจ๊ณ  ์žˆ๋Š” ๊ณต๊ธฐ ๋ถ„์ž๊ฐ€ ์–‘์„ฑ์ž ๋น”๊ณผ ์ถฉ๋Œํ•˜๋ฉด์„œ ์ผ๋ถ€ ์ด์˜จํ™”๊ฐ€ ์ง„ํ–‰๋˜๊ณ , ๋ฐœ์ƒ๋œ ์ „์ž๊ฐ€ ๋น”์˜ ๊ณต๊ฐ„ ์ „ํ•˜ ํผํ…์…œ์„ ์ƒ์‡„์‹œํ‚ค๋Š” ์ž๊ธฐ ์ค‘์„ฑํ™”(self-neutralization)์ด๋‹ค. ๋น”๋ผ์ธ์˜ ์ž”๋ฅ˜ ๊ธฐ์ฒด ๋ถ„์ž์˜ ๋ฐ€๋„๊ฐ€ ์ผ์ • ์ˆ˜์ค€์ผ ๋•Œ, ๋น” ์†์‹ค ํšจ๊ณผ์— ๋Œ€๋น„ํ•ด ์ตœ์ ์˜ ์—๋ฏธํ„ด์Šค ์ƒ์Šน ์–ต์ œ ํšจ๊ณผ๋ฅผ ๋‚ผ ์ˆ˜ ์žˆ์Œ์„ ์‹คํ—˜์ ์œผ๋กœ ํ™•์ธํ•œ๋‹ค. 3์ฐจ์› ์ž”๋ฅ˜ ๋ถ„์ž ๊ฑฐ๋™ ํ•ด์„์„ ํ†ตํ•ด ๋น” ์ˆ˜์†ก๊ด€์—์„œ ์ˆ˜์†Œ ๋ถ„์ž์™€ ๊ณต๊ธฐ ๋ถ„์ž์˜ ๋ถ€๋ถ„ ์••๋ ฅ์„ ๋‚ฎ์ถ”๊ณ , ๋น„ํ™œ์„ฑ ๊ธฐ์ฒด ๋ถ„์ž์˜ ๋ถ€๋ถ„ ์••๋ ฅ์„ ๋†’์ด๋Š” ์‹œ๋‚˜๋ฆฌ์˜ค์˜ ํšจ๊ณผ๋ฅผ ๊ณ„์‚ฐํ•ด๋ณด๊ณ , ์‹คํ—˜์—์„œ ํฌ๋ฆฝํ†ค ๊ฐ€์Šค 1.2 sccm ์ฃผ์ž… ์‹œ ์ตœ๋Œ€ ์•ฝ 23%์˜ ๋น” ์—๋ฏธํ„ด์Šค ๊ฐœ์„  ํšจ๊ณผ๋ฅผ ์–ป์—ˆ๋‹ค. ๋‘ ๋ฒˆ์งธ ๊ฒฐ๊ณผ๋กœ, ๊ธฐ๊ณ„ ํ•™์Šต ๊ธฐ๋ฒ• ์ค‘ ์ธ๊ณต ์‹ ๊ฒฝ๋ง ๋ชจํ˜•์„ ๊ธฐ๋ฐ˜์œผ๋กœ ๋น” ํŠœ๋‹์˜ ์†๋„์™€ ์ •ํ™•๋„๋ฅผ ๊ฐœ์„ ํ•˜์˜€๋‹ค. ๋น” ์ธ์ถœ, ์ง‘์†, ๊ทธ๋ฆฌ๊ณ  ํŽธํ–ฅ๊ณผ ๊ฐ™์ด ๋น” ์ˆ˜์†ก ๊ณผ์ •์— ๊ด€์—ฌ๋˜๋Š” ์š”์†Œ๋“ค ์‚ฌ์ด์—๋Š” ์ธก์ •ํ•˜๊ธฐ ์–ด๋ ค์šด ์ •๋ ฌ ์˜ค์ฐจ ๋“ฑ์˜ ๋ฏธ์ง€์ˆ˜๋“ค์ด ์กด์žฌํ•œ๋‹ค. ์ด ์˜ค์ฐจ๋ฅผ ๋ณด์ƒํ•ด์ฃผ๊ธฐ ์œ„ํ•ด ํŽธํ–ฅ ์ „์ž์„์„ ์‚ฌ์šฉํ•œ๋‹ค. ์ด ๊ณผ์ •์—์„œ ๋น” ์ˆ˜์†ก์„ ์ตœ์ ํ™”ํ•˜๊ธฐ ์œ„ํ•ด์„œ ์—ฌ๋Ÿฌ ์ „์ž์„ ์„ค์ • ๊ฐ’์— ๋Œ€ํ•ด ์ธก์ •๋˜๋Š” ๋น”์˜ ๋ณ€ํ™” ๊ทœ์น™์„ ๊ด€์ฐฐํ•˜๊ณ  ๊ทธ ์ž๋ฃŒ๋“ค์„ ํ™œ์šฉํ•  ํ•„์š”๊ฐ€ ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ๋น„์„ ํ˜•์ ์ธ ๊ด€๊ณ„๋ฅผ ์ธก์ • ์ž๋ฃŒ๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•ด์„ํ•˜๊ธฐ ์œ„ํ•ด ๋‹ค์ธต ํผ์…‰ํŠธ๋ก  ๋ชจํ˜•์„ ์ด์šฉํ•œ๋‹ค. ๋จผ์ € ์˜ˆ์ธก ๋ชจํ˜•์„ ํšจ์œจ์ ์œผ๋กœ ํ›ˆ๋ จ์‹œํ‚ค๊ณ  ๊ทธ ์‹ค์šฉ์„ฑ์„ ๋Œ€ํ•ด ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•ด ๋น” ๋™์—ญํ•™ ๊ธฐ๋ฐ˜์˜ ๊ณ„์‚ฐ์„ ์ˆ˜ํ–‰ํ•œ๋‹ค. ์ €์—๋„ˆ์ง€ ๋น” ์ˆ˜์†ก๊ณ„์—์„œ ์ผ์–ด๋‚  ์ˆ˜ ์žˆ๋Š” ์—ฌ๋Ÿฌ ๊ฐ€์ง€ ์˜ค์ฐจ ์š”์ธ๊ณผ ๋ฏธ์ง€์ˆ˜๋“ค์˜ ๋ณ€ํ™”์— ๋”ฐ๋ผ ํŠน์ • ์œ„์น˜์—์„œ์˜ ๋น” ํฌ๊ธฐ์™€ ๋น” ์œ„์น˜๋ฅผ ๊ณ„์‚ฐํ•œ ๊ฒฐ๊ณผ๋ฅผ ์–ป๋Š”๋‹ค. ์ด๋ฅผ ๋ฐ”ํƒ•์œผ๋กœ ์ถฉ๋ถ„ํ•œ ์ธก์ • ์ž๋ฃŒ๋กœ๋ถ€ํ„ฐ ์ •ํ™•๋„๊ฐ€ ๋†’์€ ์˜ˆ์ธก ๋ชจํ˜•์„ ๋„์ถœํ•  ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ•˜๊ณ , ์‹ค์ œ ๋น” ์ง„๋‹จ๊ณผ ๋น” ์ œ์–ด ์‹คํ—˜์— ์ ์šฉํ•œ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ ๊ฐœ๋ฐœํ•œ ์ธ๊ณต์‹ ๊ฒฝ๋ง ๋ชจํ˜•์€ ์ „์ž์„ ๊ฐ’์„ ์ผ์ • ๊ฐ„๊ฒฉ์œผ๋กœ ๊ฑด๋„ˆ๋›ฐ์–ด ์„ค์ •ํ•˜๋ฉฐ ๋น” ์œ„์น˜ ๋ณ€ํ™”๋ฅผ ์ธก์ •ํ•˜๋Š” ๊ธฐ์กด์˜ ์Šค์บ” ๋ฐฉ๋ฒ•์— ๋น„ํ•ด 49 ๋ฐฐ ์ด์ƒ ๋น ๋ฅธ ์†๋„๋กœ ๋” ์ •ํ™•ํ•œ ๋น” ํŠœ๋‹ ์„ฑ๋Šฅ์„ ๋ณด์ธ๋‹ค. ๋ณธ ์—ฐ๊ตฌ๋Š” ๊ณ ์ถœ๋ ฅ ์–‘์„ฑ์ž ์ž…์‚ฌ๊ธฐ์˜ ์ค‘์š” ์„ฑ๋Šฅ ์š”์†Œ์ธ ๋น” ์—๋ฏธํ„ด์Šค์˜ ์„ฑ์žฅ ์–ต์ œ์™€, ๋น ๋ฅด๊ณ  ์ •ํ™•ํ•œ ๋น” ์ˆ˜์†ก ์ œ์–ด ๊ธฐ๋ฒ• ๊ฐœ๋ฐœ์— ๊ธฐ์—ฌํ•˜์˜€๋‹ค. ์ด๊ฒƒ์€ ๊ฐ€์†๊ธฐ ๋น” ๋™์—ญํ•™ ์—ฐ๊ตฌ์— ๋น”์ง„๋‹จ ์ž๋ฃŒ์˜ ํ™œ์šฉ์„ฑ์„ ๋†’์—ฌ ๋‹ค์–‘ํ•œ ์กฐ๊ฑด์˜ ๋น”๋ผ์ธ์—์„œ ๋น” ์—๋ฏธํ„ด์Šค ํ‰๊ฐ€์™€ ํ–ฅ์ƒ์— ์ ์šฉ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ €์—๋„ˆ์ง€ ๋น” ์ˆ˜์†ก ๊ณ„ํ†ต๋ณด๋‹ค ์ œ์–ด ๋ณ€์ˆ˜๊ฐ€ ๋” ๋งŽ๊ณ  ๋ณต์žกํ•œ ๊ณ ์—๋„ˆ์ง€ ๊ฐ€์†๋‹จ๊ณผ ๋น”๋ผ์ธ์— ํ™•์žฅ ์ ์šฉํ•จ์œผ๋กœ์จ ๋น” ํŠœ๋‹ ํšจ์œจ์„ฑ์„ ํฌ๊ฒŒ ๊ฐœ์„ ํ•  ๊ฐ€๋Šฅ์„ฑ์ด ์žˆ๋‹ค. ๊ถ๊ทน์ ์œผ๋กœ๋Š” ์šด์ „์ž์˜ ๊ฐœ์ž…์„ ์ตœ์†Œํ™”ํ•˜๋Š” ๊ฐ€์†๊ธฐ ์ž์œจ ์šด์ „์˜ ๊ธฐ๋ฐ˜ ๊ธฐ์ˆ ๋กœ ๋ฐœ์ „์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค.Chapter 1. Introduction 1 1.1. High Intensity Proton Injector 1 1.2. Applications of High Intensity Proton Injector 4 1.3. Previous Work and Research Motivation 11 1.4. Contribution and Scope of the Study 14 Chapter 2. Theoretical Background 18 2.1. Ion Source for High-Intensity Proton Injector 18 2.2. Beam Formation and Extraction 24 2.3. Beam Parameters and Beam Dynamics 27 2.4. Low Energy Beam Transport and Beam Matching 32 2.5. Beam Diagnostics for the Low Energy Beam 36 2.6. Machine Learning and its Application in Accelerator Control 40 Chapter 3. Experimental Setup of Proton Injector Test Stand 46 3.1. Microwave Ion Source and Beam Extraction System 46 3.2. Low Energy Beam Transport System 59 3.3. Low Energy Beam Diagnostics 69 Chapter 4. Beam Emittance Measurement and Mitigation of Emittance Growth 74 4.1. Space Charge Effect and Self-Neutralization 74 4.2. Numerical Analysis on Residual Gas Molecules 78 4.3. Transverse Beam Emittance Measurement with Solenoid Scan Method 85 4.4. Mitigation of Emittance Growth by Enhanced Self-Neutralization 92 Chapter 5. Tuning of the Beam Parameters by Artificial Neural Network Model 97 5.1. Beam Dynamics Simulations: Training Data Preparation 97 5.2. Artificial Neural Network Model for the Fast Beam tuning 101 5.3. Experimental Validation and Application on Beam Control Experiment 109 Chapter 6. Conclusion and Future Work 116 6.1. Conclusive Summary of the Study 116 6.2. Recommendations for Future Work 119 Bibliography 121 Abstract in Korean 129๋ฐ•

    The effects of macrophage-stimulating protein and gamma synuclein on the development of brainstem motor systems

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    Disorders of motility are among the most common and debilitating neurological ailments. In most cases, treatment of these conditions is at best palliative. This is mainly due to the apparent inability of central neurons to regenerate after a given noxious event. In the past, embryos have proven to be valuable objects to study the mechanisms of growth and death in nerve cells since both are physiological events in the developing nervous system. The discovery and study of an ever-growing list of molecules that are involved in these events has significantly furthered our understanding of the conditions that have to be met for individual nerve cell populations to develop into functional structures. It also has the potential to contribute significantly to the establishment of more targeted and efficient therapeutic strategies.Here, the effects of macrophage-stimulating protein (MSP) and 7- synuclein on two systems in the developing brainstem involved in controlling movement have been studied: a) the cranial motoneurons and b) the dopaminergic neurons of the substantia nigra and the ventral tegmental area. MSP exerts a variety of biological actions on many cell types, but has no known functions in the brain. To investigate whether MSP is also capable of acting as a neurotrophic factor, hypoglossal motoneurons were purified from the embryonic chicken hindbrain because these neurons are known to express the MSP receptor tyrosine kinase RON. The study shows that MSP promotes the in vitro survival of these neurons during the period of naturally occurring neuronal cell death and enhances the growth of neurites from these neurons. Furthermore, MSP mRNA was detected in the developing tongue which is the XXI target tissue for hypoglossal neurons. These studies demonstrate that MSP is a neurotrophic factor for a distinct population of developing motoneurons.ฮณ-synuclein is a recently discovered member of the synuclein family. Another member of this family, a-synuclein has been implicated in the pathogenesis of Parkinson's disease. However, little is known about the function of ฮณ-synuclein and it has not yet been directly implicated in the genesis of neurodegenerative conditions. Here, brainstems of transgenic mice lacking ฮณ-synuclein have been analysed by means of immunohistochemical and histological techniques. The data obtained shows that ฮณ-synuclein is expressed in the murine substantia nigra and in most cranial motor nuclei and that the localization of the protein undergoes a shift during development from a cytosomal to an axonal and synaptic localization. Mice lacking ฮณ-synuclein have a deficit of neurons in these structures. In the context of recent studies which have revealed in vivo and in vitro interactions between the synucleins, this data suggests that a fine balance between ฮฑ- and ฮณ-synuclein seems critical to prevent the demise of certain neurons during the period of naturally occurring neuronal cell death. It also indicates that ฮณ-synuclein may play a role in the pathogenesis of Parkinson's diseas

    Doctor of Philosophy

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    dissertationOptical methods are well-established in the fields of neuroscience, medical imaging, and diagnostics, etc. Optogenetics, for example, enables molecular specificity in optical neural stimulation and recording and has been named the "Method of the Year 2010" by Nature Methods. A novel microdevice was designed, fabricated, developed, and tested to facilitate three-dimensional (3D) deep-tissue light penetration with the capacity to accommodate spatiotemporal modulation of one or more wavelengths to advance a broad range of applications for optical neural interfaces. A 3D optrode array consisting of optically transparent "needles" can penetrate >1 mm directly into tissue, thereby creating multiple independent paths for light propagation that avoid attenuation due to tissue absorption and scattering, providing a high level of selectivity and comprehensive access to tissue not available in current interfaces. Arrays were developed based upon silicon and glass. The silicon optrode array is based upon the well-established Utah electrode array architectures and is suitable for near-infrared (NIR) applications; glass optrodes are appropriate waveguides for both visible and NIR wavelengths. Arrays were bulk-micromachined with high-aspect ratio, a process that has not been reported to be applied to glass previously. In addition to device fabrication, extensive laboratory testing was performed with various optical sources to determine loss mechanisms and emitted beam profiles in tissue across the relevant wavelength ranges, with particular focus on performance metrics for optogenetic and infrared neural stimulation applications. Optrode arrays were determined to be amenable to integration with typical neural stimulation and imaging light delivery mechanisms such as optical fibers and microscopes. Glass optrodes were able to transmit light at ~90% efficiency through depths many times greater than the tissue attenuation length, with negligible light in-coupling loss. Si optrodes were determined to be only ~40% efficient with losses mostly from high index contrast, tip backreflection, and taper radiation. The in-coupling technique and optrode geometry may be modified to produce illumination volumes appropriate for various experimental paradigms. While the focus of this work is on optical neural stimulation, optrode array devices have application in basic neuroscience research, highly selective photodynamic therapy, and deep tissue imaging for diagnostics and therapy
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