55 research outputs found
์ด๋จ ํ์ค ์์ญ์์ ๋น์ ํ ๊ด์ฌ์ ๋ ์ด์ ์์คํ ์ ์์นํด์ ์ฐ๊ตฌ
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ผ๋ฌธ (๋ฐ์ฌ)-- ์์ธ๋ํ๊ต ๋ํ์ ๊ณต๊ณผ๋ํ ์ ๊ธฐยท์ปดํจํฐ๊ณตํ๋ถ, 2017. 8. ์ ์ค์ฐฌ.In this dissertation, nonlinear fiber laser systems in the sub-ps pulse regime are numerically investigated. The main research subjects of this dissertation are categorized into two groups: (1) nonlinear effects in noncavity configurations, e.g. nonlinear fiber sections pumped by ultrashort pulses and (2) nonlinear effects in cavity configurations, e.g. mode-locked fiber ring lasers. When the systems accompany large amount of nonlinearity, the nonlinear effects result in extreme spectral broadening, called supercontinuum generation (SCG) for the former case and multi-pulse operation for the latter case. By exploiting the master equations based on the nonlinear Schrรถdinger equation (NLSE), I numerically simulate the ultrashort-pulse evolution in the nonlinear fiber laser systems. By analyzing the simulation results, I optimize the system performance or verify unclarified phenomenon in the investigated systems.
In the first two parts of the dissertation, I focus on studying the SCG in noncavity configurations. First, I numerically study the dynamics of SCG for a variety of possible combinations of photonic crystal fibers (PCFs) and ultrafast fiber laser pulses that current technologies offer. Three types of PCFs typically used in SCG and four representative types of ultrafast fiber laser pulses are considered for this combinatorial study. I numerically model and qualitatively discuss the nonlinear evolution of the pulses for their 12 combinatorial cases. I also quantitatively analyze their output spectra and organize a performance chart for them in terms of spectral bandwidth, flatness, and degree of spectral coherence. Through these works, I suggest the most viable combinations among the given PCFs and ultrafast fiber laser pulses in order to generate a target SC spectrum for various specific cases.
In the second part of this dissertation, I numerically study the dynamics of SCG in a ytterbium-doped highly nonlinear PCF (HNL-PCF) in the sub-ps regime. I disucss the enhancement of the energy spectral density and the recovery of the peak power depletion in the SCG process through the fiber in comparison with the SCG based on a passive-type fiber. As a unique application of the novel characteristics of the active HNL-PCF, I also analyze the direct amplification of a SC pulse through it, showing that the incident SC pulse can be amplified by 10 dB without undergoing significant degradations in terms of spectral bandwidth and flatness. These numerical investigations on the active HNL-PCF will be helpful for opening up new opportunities for fiber-based SCG technology in the sub-ps pulse regime.
In the third part of this dissertation, I focus on the nonlinear effects in cavity configurations. I numerically investigate quasi-mode-locked (QML) multi-pulse dynamics in a fiber ring laser in the anomalous dispersion (AD) regime. I show that the laser cavity can operate in five constitutively different QML regimes, depending on the saturation power of the saturable absorber element and the length of the passive fiber section that parameterize the overall nonlinearity and dispersion characteristics of the laser cavity. I classify them into the incoherent noise-like pulse (NLP), partially-coherent NLP, symbiotic, partially-coherent multi-soliton, and coherent multi-soliton regimes, accounting for their coherence and multi-pulse formation features. In particular, I numerically clarify and confirm the symbiotic regime for the first time to the best our knowledge, in which NLP and multi-solitons coexist stably in the cavity that has recently been observed experimentally. Furthermore, I analyze the shot-to-shot coherence characteristics of the individual QML regimes relative to the amount of the nonlinear-phase shift per roundtrip, and verify a strong correlation between them. I also show that the net-cavity dispersion plays a critical role in determining the multi-pulse dynamics out of the partially-coherent NLP, symbiotic, and partially-coherent multi-soliton regimes, when the cavity bears moderate nonlinearity. I quantify and visualize all those characteristics onto contour maps, which will be very useful and helpful in discussing and clarifying the complex QML dynamics.
In the fourth part of this dissertation, I extend the analysis of the AD QML cavity into the normal-dispersion (ND) QML cavity. While adjusting two chosen cavity parameters: saturation power of the SA and the length of the ND passive fiber, I verify three distinctive QML operation regimes. Accounting for the temporal dynamics in three QML regimes, I classify them into the NLP, transient, and symbiotic regimes. In each regime, I quantitatively analyze the shot-to-shot stability of the QML pulse and its relation with the cavity nonlinearity by visualizing the results on contour maps. Finally, I discuss the origin of the degradation of the shot-to-shot stability in the ND QML cavity.Chapter 1 Introduction. 1
1.1 Overview on fiber optics 1
1.2 Motivation of this dissertation 6
1.3 Scope and organization. 10
Chapter 2 Nonlinear dynamics in noncavity configurations: supercontinuum generation. 12
2.1 Passive supercontinuum generation in the sub-ps regime. 12
2.2 Active Supercontinuum generation in the sub-ps regime 45
Chapter 3 Nonlinear dynamics in cavity configurations: quasi-mode-locked operation. 67
3.1 Quasi-mode-locked operation in an anomalous dispersion cavity. 67
3.2 Quasi-mode-locked operation in a normal dispersion cavity 92
Chapter 4 Conclusion. 106
Bibliography. 112
ํ๊ธ ์ด๋ก. 120Docto
์ด๋๊ฐ์ฒด ๋ฐ์ดํ๋ฒ ์ด์ค์์ TP ์ต๊ทผ์ ์ ์ง์์ ์ฒ๋ฆฌ
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ผ๋ฌธ(์์ฌ)--์์ธ๋ํ๊ต ๋ํ์ :์ ๊ธฐยท์ปดํจํฐ๊ณตํ๋ถ,2004.Maste
Experimental investigation on the turbulent structure of elliptic jets by using a 3-D LDV system
Maste
Plasma Arc Curing light ์ผ๋ก ๊ด์กฐ์ฌํ ์์์ง ์ ์ฐฉ์ ์ ์ ๋จ์ ์ฐฉ๊ฐ๋
Thesis(master`s)--์์ธ๋ํ๊ต ๋ํ์ :์น์ํ๊ณผ ์น๊ณผ๋ณด์กดํ์ ๊ณต,2007.Maste
๋ณตํฉ๋ ์ง์ ์ถฉ์ ๋ฐฉ๋ฒ์ด ์คํฉ์์ถ์๋ ฅ์ ๋ฏธ์น๋ ์ํฅ
Objective: The aim of this study was to investigate the effect of layering methods using a methacrylate-based composite, a flowable composite liner and a low shrinkage silorane-based composite on the polymerization shrinkage stress of light cured composites.
Methods: Twenty four aluminum blocks were used to prepare MOD cavities and divided into four groups. A universal hybrid methacrylate-based Filtek Z250 composite (Z250), a Filtek Z350 flowable composite (Z350 flowable), and a silorane-based Filtek P90 composite (P90) were used to fill the cavities. Cavities were restored using four different filling protocols. Group 1 was filled in bulk with Z250, group 2 was restored by an increment technique with the same composite, group 3 by an increment technique with Z250 after lining with a Z350 flowable, and group 4 by an increment technique with P90. The axial shrinkage strain and flexural modulus of the three composites were determined, and cuspal deflection of each group was measured with LVDT probes and compared among groups using ANOVA and Tukeys post hoc test (ฮฑ=0.05).
Results: The axial shrinkage strains of P90, Z250, and Z350 flowable were 1.05 (0.09), 2.28 (0.04), and 4.12 (0.09)%, respectively. The flexural modulus of P90 was 10.1 (0.9), Z250 was 13.6 (2.0), and Z350 was 7.6 (0.9) GPa. The cuspal deflections at 33 minutes in groups 1-4 were 18.2 (1.54), 14.5 (0.47), 16.2 (1.10), and 6.6 (0.44) ใ, respectively. The increment technique yielded significantly lower cuspal deflection than the bulk technique. Flowable composite lining under incrementally filled universal composite (Z250) showed higher cuspal deflection than that without flowable composite lining. Silorane-based (P90) composite exhibited lower cuspal deflection than methacrylate-based (Z250) composite.
Significance: Cuspal deflection resulting from polymerization shrinkage stress can be reduced by the increment technique and low shrinking composite to obtain optimal clinical outcomes. Flowable composite lining under incrementally filled universal composite did not reduce polymerization shrinkage stress in terms of cuspal deflection.๋ชฉ์ : ๋ณธ ์ฐ๊ตฌ์ ๋ชฉ์ ์ ์ ์ธต์ถฉ์ ๋ฐฉ๋ฒ, flowable ๋ณตํฉ๋ ์ง ์ด์ฅ์ฌ์ ์ฌ์ฉ ๋ฐ ์ ์์ถ silorane-based ๋ณตํฉ๋ ์ง ์ฌ์ฉ์ด ๊ด์คํฉ ๋ณตํฉ๋ ์ง์ ์คํฉ์์ถ์๋ ฅ์ ๋ฏธ์น๋ ์ํฅ์ ์กฐ์ฌํ๊ธฐ ์ํจ์ด๋ค.
์ฌ๋ฃ ๋ฐ ์ฌ์ฉ๋ฐฉ๋ฒ: MOD ์๋์ด ํ์ฑ๋ 24๊ฐ์ ์๋ฃจ๋ฏธ๋ ๋ธ๋ก์ ์ ์ํ์ฌ ๋ค ๊ตฐ์ผ๋ก ๋ถ๋ฅํ์๋ค. ์ถฉ์ ์ ์ฌ์ฉ๋ ๋ณตํฉ๋ ์ง์ methacrylate-based ์ ๊ตฌ์น ๋ฒ์ฉ ๋ณตํฉ๋ ์ง (Z250), flowable ๋ณตํฉ๋ ์ง (Z350 flowable), silorane-based ๋ณตํฉ๋ ์ง (P90) ์ด์๊ณ , ํ์ฑ๋ ์๋์ ๊ตฐ๋ณ๋ก ๋ค ๊ฐ์ง ๊ฐ๊ธฐ ๋ค๋ฅธ ์ถฉ์ ๋ฐฉ๋ฒ์ผ๋ก ์ถฉ์ ๋์๋ค. 1๊ตฐ์ Z250 ๋ณตํฉ๋ ์ง์ผ๋ก ํ ๋ฒ์ ์ถฉ์ ํ์๊ณ , 2๊ตฐ์ Z250 ๋ณตํฉ๋ ์ง์ผ๋ก ์ ์ธต ์ถฉ์ ํ์๋ค. 3๊ตฐ์ Z350 flowable ๋ณตํฉ๋ ์ง์ผ๋ก ์ด์ฅ ํ Z250์ผ๋ก ์ ์ธต ์ถฉ์ ํ์๊ณ 4๊ตฐ์ P90์ผ๋ก ์ ์ธต ์ถฉ์ ํ์๋ค. ์ธ ์ข
์ ๋ณตํฉ๋ ์ง์ axial ์คํฉ์์ถ๋ฅ ๊ณผ ๊ตด๊ณก ํ์ฑ๊ณ์๋ฅผ ์ธก์ ํ์๊ณ , LVDT probe๋ฅผ ์ฌ์ฉํ์ฌ ๊ฐ ๊ตฐ์์ ๊ต๋๊ตด๊ณก์ ์ธก์ ํ์์ผ๋ฉฐ, ANOVA์ Tukeys post hoc test๋ก ๋ถ์ํ์๋ค (ฮฑ=0.05).
๊ฒฐ๊ณผ: P90, Z250, ๊ทธ๋ฆฌ๊ณ Z350 flowable ์ axial ์คํฉ์์ถ๋ฅ ์ ๊ฐ๊ฐ 1.05 (0.09), 2.28 (0.04), 4.12 (0.09)% ์๋ค. P90์ ๊ตด๊ณก ํ์ฑ๊ณ์๋ 10.1 (0.9), Z250์ 13.6 (2.0), ๊ทธ๋ฆฌ๊ณ Z350์ 7.6(0.9) GPa ๋ก ๊ฐ์ฅ ๋ฎ์๋ค. 1๊ตฐ์์ 4๊ตฐ์ ํ๊ท ๊ต๋๊ตด๊ณก์ ๊ด์กฐ์ฌ ์์ ํ 33๋ถ์์ ๊ฐ๊ฐ 18.2 (1.54), 14.5 (0.47), 16.2 (1.10), 6.6 (0.44) ใ ์ด์๋ค. ์ ์ธต ์ถฉ์ ์ด ํ ๋ฒ์ ์ถฉ์ ๋ณด๋ค ํ์ ํ ์ ์ ๊ต๋๊ตด๊ณก์ ๋ณด์๋ค. Z250 ๋ณตํฉ๋ ์ง์ผ๋ก ์ ์ธต ์ถฉ์ ํ๊ธฐ ์ ์ flowable ๋ณตํฉ๋ ์ง์ ์ด์ฉํ์ฌ ์ด์ฅํ ๊ฒฝ์ฐ, flowable ๋ณตํฉ๋ ์ง ์ด์ฅ์ฌ ์์ด Z250 ์ผ๋ก๋ง ์ ์ธต ์ถฉ์ ํ ๊ฒฝ์ฐ๋ณด๋ค ๋ ํฐ ๊ต๋๊ตด๊ณก์ ๋ณด์๋ค. Silorane-based ๋ณตํฉ๋ ์ง (P90) ์ด methacrylate-based ๋ณตํฉ๋ ์ง์ ๊ฒฝ์ฐ (Z250) ๋ณด๋ค ๋ ์ ์ ๊ต๋๊ตด๊ณก์ ๋ํ๋๋ค.
๊ณ ์ฐฐ: ์คํฉ์์ถ์๋ ฅ์ ์ํด ๋ฐ์๋๋ ๊ต๋๊ตด๊ณก์ ์ ์ธต ์ถฉ์ ๋ฒ์ด๋ ์ ์์ถ ๋ณตํฉ๋ ์ง์ ์ฌ์ฉํ์ฌ ์ค์ผ ์ ์์๋ค. ๋ฒ์ฉ ๋ณตํฉ๋ ์ง์ผ๋ก ์ ์ธต ์ถฉ์ ํ๊ธฐ ์ ์ flowable ๋ณตํฉ๋ ์ง ์ด์ฅ์ฌ๋ฅผ ์ฌ์ฉํ๋ ๊ฒ์ ์คํฉ์์ถ์๋ ฅ์ ์ํ ๊ต๋๊ตด๊ณก์ ๊ฐ์์ํค์ง ๋ชปํ์๋ค.Docto
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