• Title/Summary/Keyword: 툴륨

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Theoretical modeling and analysis of thulium doped fluoride fiber amplifier at 1.47 $\mu\textrm{m}$ band amplification (툴륨이 첨가된 플루오르 계열의 광섬유 증폭기의 1.47$\mu\textrm{m}$ 증폭 대역에 대한 모델링과 분석에 대한 연구)

  • 이원재;민범기;박재형;박남규
    • Korean Journal of Optics and Photonics
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    • v.11 no.3
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    • pp.171-178
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    • 2000
  • We present a numerical model which enables to analyze $1.47mu$m amplification band characteristics for thulium doped fluoride fiber amplifiers. We focused on upconversion pumping scheme, thus many transitions affecting $1.47mu$m band amplification was considered simultaneously. Backward propagating waves and transverse mode were also considered in the model. The parameters for modeling were then acquired using published experimental data and related theories such as Judd-Ofelt theory for radiative transition, empirical energy gap law for non-radiative transition, and McCumber relations for cross-sections. The simulation showed well-matched results with experiment and internal dynamics. amics.

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Passively Mode-Locked 1.93-㎛ All-Fiberized Femtosecond MOPA Laser Using a Gold-Deposited Side-Polished Fiber (금 증착 측면연마 광섬유를 이용한 1.93㎛ 모드잠금 펨토초 전광섬유 MOPA 레이저)

  • Jung, Minwan;Koo, Joonhoi;Lee, Ju Han
    • Korean Journal of Optics and Photonics
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    • v.25 no.6
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    • pp.340-345
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    • 2014
  • We experimentally demonstrate the use of a gold-deposited side-polished fiber as a $2-{\mu}m$-band polarizing device to produce mode-locked pulses from a thulium/holmium-codoped fiber ring cavity. The mode-locking effect was induced by nonlinear transmission caused by the gold-deposited side-polished fiber, due to nonlinear polarization rotation of the oscillated beam within the fiberized cavity. It is also shown that ~558-fs pulses with a peak power of ~6.7 kW could readily be produced at a wavelength of 1935 nm through subsequent thulium/holmium-codoped fiber amplification, due to the higher-order soliton compression effect.

Nonstoichiometry of the Thulium Sesquioxide (산화툴륨의 비화학양론)

  • Chul Hyun Yo;Eun Seok Lee;Woong Bum Pyon;Jae Shi Choi;Moo Sil Pyon
    • Journal of the Korean Chemical Society
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    • v.33 no.1
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    • pp.25-30
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    • 1989
  • The nonstoichiometry and electrical conductivities of Tm$_2O_3$ were studied in the oxygen pressure $2\;{\times}\;10^{-1}\;-1\;{\tiems}\;10^{-4}$ atm under the temperature ranges from 700 to 1100$^{\circ}$C. The x values of $TmO_{1.5+X}$ were varied in the ranges of 0.1004∼0.0110. The enthalpies of formation of the nonstoichiometric compounds were found to be 5.40-4.71 kcal/mole, and the average activation energy obtained from the plots of log conductivity vs. 1000/T was 1.65 eV. The Po$_2$ dependencies of the electrical conductivity were found to be linear and closely approaximated to ${\sigma}{\alpha} PO{\frac{1}{2}^{/5.3}$ in the temperature range 700∼1100$^{\circ}$C. The nonstoichiometry and the electrical conductivity are due to trivalent metal vacancies.

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A Comparative Study of Branching Ratio of 167Yb Radioactive Isotope from Gamma-ray Spectrum Produced by 169Tm(p,3n)167Yb Reaction with 100-MeV Proton Beam (100-MeV 양성자 빔을 이용하여 169Tm(p,3n)167Yb 반응에 의해 생성된 167Yb 방사성동위원소에서 방출되는 감마선 스펙트럼 비교 연구)

  • Sam-Yol, Lee
    • Journal of the Korean Society of Radiology
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    • v.16 no.7
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    • pp.953-960
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    • 2022
  • The measurement of branching ratio of 167Yb radioactive isotopes from gamma-ray spectrum of 169Tm(p,3n)167Yb reaction were performed by using a 100-MeV proton linear accelerator of the Korea Multi-purpose Accelerator Complex (KOMAC). The 167Yb isotope has a half-life of 17.5 minutes and decays to 169Tm. The gamma rays generated from the 167Yb isotope were measured using an HPGe detector gamma ray spectroscopy system. The energy calibration of the detector and the efficiency measurement of the detector were determined using a standard source. The gamma rays of known main energy (62.9, 106.2, 113.3, 143.5 and 176.3 keV) were measured. On the other hand, information about the intensity of the generated gamma rays is very inaccurate. Therefore, in this study, the decay strength of the main gamma rays was accurately measured. Overall, it was different from the previously known results, and in particular, it was found that the intensity of the main decay gamma ray, such as the 113.3 and 106.2 keV gamma ray, was overestimated, and it was found that the gamma ray, such as 62.9, 116.7 and 143.5 keV was underestimated. The present results are considered to be important information in the fields of nuclear fusion, astrophysics and nuclear physics in the future.