• 천문학회보
• /
• 제41권1호
• /
• pp.70.3-70.3
• /
• 2016

Active galactic nuclei (AGNs) typically show a non-thermal continuum locally represented by a power-law and many prominent emission lines in the UV and optical regions. AGNs are classified by two types, where Type I AGNs exhibit both broad and narrow lines and only narrow lines are observed in Type 2 AGNs. The unification models of AGNs invoke the existence of a molecular torus just outside of the broad line region. In the presence of a high column HI region associated with the molecular torus, we propose that significant fraction of broad line photons near Lyman series can be scattered by atomic hydrogen in the torus. In particular, $Ly{\alpha}$ being the strongest emission line, strong linear polarization may develop around $Ly{\alpha}$ through Rayleigh scattering. We adopt a Monte Carlo technique to investigate the polarized transfer of $Ly{\alpha}$ in a thick HI region with the shape of a torus. We consider the range of HI column density N_HI = 1020-23 with fixed geometric parameters of the torus such as the inner and outer radii and the height. We present the polarized spectra and angular distribution of Rayleigh scattered radiation around $Ly{\alpha}$. We find that the $Ly{\alpha}$ core part is polarized in the direction perpendicular to the symmetry axis whereas in the far wing part it is polarized in the parallel direction. It is concluded that the unification of AGNs implies that $Ly{\alpha}$ can be uniquely polarized through Rayleigh scattering.

• 전자공학회논문지D
• /
• 제35D권12호
• /
• pp.59-67
• /
• 1998

본 논문에서는 몬테카를로 방식을 사용하여 이온의 에너지에 대한 타겟 원자의 스퍼터율(Sputter Yield), 이온의 주입 각도에 대한 스퍼터율, 이온의 주입에 따른 타겟 원자의 발산 분포를 3차원으로 시뮬레이션 하였다. 중(중)이온으로 (Ar/sup +/)을 사용하였고, 경(輕)이온으로 (H/sup +/)을 사용하여 10 eV에서 100 KeV 영역의 에너지에 따른 스퍼터율을 계산하였다. 또한, 스퍼터 타겟 물질로서 Cu, Al을 사용하여 계산하였고, 실험치와 일치함을 확인하였다. 스퍼터율은 입사 이온의 에너지가 증가함에 따라 증가하는 경향을 보이지만, 임계점 이후에는 점차적으로 감소하는 경향을 보였다. 중이온에 의한 스퍼터에서는 임계점이 10 KeV 영역이었고, 경이온에 의한 스퍼터에서는 1 KeV 이하 영역이었다. 또한, 이온의 주입 각도에 따라서 타겟의 스퍼터율은 점차적으로 증가하였고, 68° 부근에서 최대 스퍼터율을 기록하였다. 이온의 주입 각도에 따른 타겟 원자의 분포도에서는 각도가 커짐에 따라서 타겟 표면 법선 방향으로 방출되는 원자의 수가 많아짐을 확인하였다. 본 연구에서는, CRAY T3E 슈퍼컴퓨터에서 시뮬레이션을 수행하였으며, 구현된 몬테카를로 스퍼터 시뮬레이터의 GUI(Graphic User Interface) 환경을 구축하였다.

• The Journal of Advanced Prosthodontics
• /
• 제5권1호
• /
• pp.58-66
• /
• 2013

PURPOSE. The purpose of this study was to decide the most appropriate point on tragus to be used as a reference point at time of marking ala tragus line while establishing occlusal plane. MATERIALS AND METHODS. The data was collected in two groups of subjects: 1) Dentulous 2) Edentulous group having sample size of 30 for each group with equal gender distribution (15 males, 15 females each). Downs analysis was used for base value. Lateral cephalographs were taken for all selected subjects. Three points were marked on tragus as Superior (S), Middle (M), and Inferior (I) and were joined with ala (A) of the nose to form ala-tragus lines. The angle formed by each line (SA plane, MA plane, IA plane) with Frankfort Horizontal (FH) plane was measured by using custom made device and modified protractor in all dentulous and edentulous subjects. Also, in dentulous subjects angle between Frankfort Horizontal plane and natural occlusal plane was measured. The measurements obtained were subjected to the following statistical tests; descriptive analysis, Student's unpaired t-test and Pearson's correlation coefficient. RESULTS. The results demonstrated, the mean angle COO (cant of occlusal plane) as $9.76^{\circ}$, inferior point on tragus had given the mean angular value of IFH [Angle between IA plane (plane formed by joining inferior point-I on tragus and ala of nose- A) and FH plane) as $10.40^{\circ}$ and $10.56^{\circ}$ in dentulous and edentulous subjects respectively which was the closest value to the angle COO and was comparable with the values of angle COO value in Downs analysis. Angulations of ala-tragus line marked from inferior point with occlusal plane in dentulous subject had given the smallest value $2.46^{\circ}$ which showed that this ala-tragus line was nearly parallel to occlusal plane. CONCLUSION. The inferior point marked on tragus is the most appropriate point for marking ala-tragus line.

• 대한조선학회논문집
• /
• 제34권1호
• /
• pp.68-76
• /
• 1997

본 논문에서는 선박 및 해양 구조물을 구성하는 용접 판구조물의 변형 및 잔류응력 등 용접 초기 결함을 효율적으로 평가할 수 있는 열탄소성 해석방법을 정립하였다. 또한 평판의 선상가열공법(line heating process)을 열탄소성 시뮬레이션함으로써 작업의 고능률화 및 자동화를 위한 기초연구를 수행하였다. 판구조물에 대한 열전도 해석을 수행하기 위하여 해석적인 방법과 수치적인 방법을 병행하였다. 판구조물의 열탄소성 해석방법에 있어서는 초기변형도법에 근거한 유한요소법을 사용하였으며, 증분 구간중 소성 구역에서는 응력 증분 및 항복응력 중분의 2 차항까지 고려해서 시간 증분을 최적 제어함으로써 해석 불능에 빠지는 문제를 극복하였다. 특히 응력 중분에 탄성계수의 온도에 따른 증분을 2 차항까지 포함시켰다. 평판의 두께와 입열량을 변화시키면서 일련의 용접 열탄소성 실험을 수행하였는 바, 온도 및 용접 변형을 계측하여 수치 계산 결과와 비교하여 상호 부합성이 양호함을 확인하였다.

• 대한원격탐사학회지
• /
• 제8권2호
• /
• pp.93-104
• /
• 1992

현재 한국표준지형도에서 사용되고 있는 횡단메카토르좌표(TM) 체제는 한반도 전체를 단일의 직각좌표 체계로 표시하는데 제한이 있다. 인공위성 원격탐사 및 지리정보 시스템의 광범 위한 응용과 함께, 직각좌표체계가 종래의 경위도좌표체계보다 이용에 있어서 보다 편리하고 효 과적이라 할 수 있다. 본 논문에서는 한반도 전체를 하나의 좌표구역으로 포함하는 통합된 직각 좌표체계를 제안함으로써 표준직각좌표체계 설정의 기반을 도모하고자 하였다. 표준지형도 제작 에 사용된 횡단메카토르 투영법을 그대로 유지하고, 기존의 TM좌표 및 UTM좌표를 약간 변형하 여 기준원점이 동경 127$^{\circ}$30'와 북위 38$^{\circ}$가 되는 직각좌표체계를 시도하였다. 경위도 좌표 에서 통합된 직각좌표로의 변환과정을 축척오차의 분포 문제와 함께 기술하였다.

• Bulletin of the Korean Chemical Society
• /
• 제16권12호
• /
• pp.1193-1203
• /
• 1995

In this work, we focused on the setup of the tools for the analysis of the final rotational state distribution of photofragments in vibrational predissociations of triatomic van der Waals molecules A-B2. We found that reflection principle used for the direct photodissociation processes can also be applied to find out the final rotational state distributions for indirect photodissociation processes. The quantity which represents the strength of rovibrational coupling between the quasi-bound state and the final state is reflected into the mirror of the classical angular momentum function, instead of the initial state before light absorption used in the reflection principle of direct processes. The sign change in the first derivative of the interaction potential with respect to the bond distance of B2 is found to be the source of the binodal structures in the final rotational distributions of photofragments in the model system studied in this work. In MQDT analysis, short range eigenchannel basis functions were found to be localized in angle, in the previous work [Lee, C.W. Bull. Korean Chem. Soc. 1995, 16, 957.] and may be called angle functions. Angle functions enjoy simple geometrical structures which have simple functional relations with the final state distributions of photofragments. Two processes take place along the angle functions which resemble the quasi-bound state and dominate over other processes. Two such angle functions are found to be not only localized angularly but also localized either one of ends of B2 in motions along the bond of B2. These dominating photodissociation processes, however, cancel each other. This cancellation causes photodissociation to depend sensitively on the interaction potential at other angles than the dominant one. Part of potential surface where much larger torque exists can now play an important role in photodissociation. MQDT also enables us to see which processes play important roles after cancellation. This is done by examining the amounts of time delayed by asymptotic eigenchannels.

• Bulletin of the Korean Chemical Society
• /
• 제18권12호
• /
• pp.1274-1280
• /
• 1997

The photodissociation dynamics of CH2I2 has been studied at 304 nm by state-selective photofragment translational spectroscopy. Velocity distributions, anisotropy parameters, and relative quantum yields are obtained for the ground I(2P3/2) and spin-orbit excited state I*(2P1/2) iodine atoms, which are produced from photodissociation of CH2I2 at this wavelength. These processes are found to occur via B1 ← A1 type electronic transitions. The quantum yield of I*(2P1/2) is determined to be 0.25, indicating that the formation of ground state iodine is clearly the favored dissociation channel in the 304 nm wavelength region. From the angular distribution of dissociation products, the anisotropy parameters are determined to be β(I)=0.4 for the I(2P3/2) and β(I*)=0.55 for the I*(2P1/2) which substantially differ from the limiting value of 1.13. The positive values of anisotropy parameter, however, show that the primary processes for I and I* formation channels proceed dominantly via a transition which is parallel to I-I axis. The above results are interpreted in terms of dual path formation of iodine atoms from two different excited states, i.e., a direct and an indirect dissociation via curve crossing between these states. The translational energy distributions of recoil fragments reveal that a large fraction of the available energy goes into the internal excitation of the CH2I photofragment; < Eint > /Eavl=0.80 and 0.82 for the I and I* formation channels, respectively. The quantitative analysis for the energy partitioning of available energy into the photofragments is used to compare the experimental results with the prediction of direct impulsive model for photodissociation dynamics.

• 한국광학회지
• /
• 제3권3호
• /
• pp.161-166
• /
• 1992

회전하는 거친금속표면에 s-편극된 레이저광을 $-30^{\circ}$로 입시시켜 생긴 후방산란파중 입사광과 동일한 편극을 가지는 후방산란파에 대하여 세기의 시간상관함수 $g_{s}^{(2)}(\tau)$를 측정하였다. 이 과정에서 광전신호로부터 $g_{s}^{(2)}(0)$의 측정을 할 때 수반되는 shot noise의 영향을 제하여 줌으로써 정확한 $g_{s}^{(2)}(0)$ 값을 얻었다. 각 산란각$\theta_{s}$에서$g_{s}^{(2)}(\tau)$는 {1+exp($-\tau^2/\tau_0^2$)}함수와 거의 일치하였는데, 이는 등속으로 회전하는 간유리를 투과하여 형성된 레이저 스펙클의 경우와 같은 결과이다. 또한, 산란각에 따른 $\tau_0$의 분포에서는 $\theta_s=34^{\circ}$에서 예리하게 최대값을 가지는 것이 관찰되었다. 이 연구에서, 다중산란이 10%를 넘는 금속판산란과 다중산란이 무시될 수 있는 간유리판산란이 같은 함수꼴의 세기의 시간상관함수를 갖는다는 사실이 확인되었다.

• 천문학회지
• /
• 제54권6호
• /
• pp.171-182
• /
• 2021

The lack of short baselines, referred to as the short-spacing problem (SSP), is a well-known limitation of the performance of radio interferometers, causing a reduction of the flux detected from source structure on large angular scales. The very large number of antennas operated in the Atacama Large Millimeter/sub-millimeter Array (ALMA) generates situations for which the impact of the SSP takes a complex form, not simply measurable by a single number, such as the maximal recoverable scale. In particular, extended antenna configurations, complemented by a small group of closeby antennas at the centre of the array, may result in a double-humped baseline distribution with a significant gap between the two groups. In such cases one should adopt as the effective maximal recoverable scale the one associated with the extended array and use only the central array to recover missing flux, as one would do with single dish or ACA (Atacama Compact Array) observations. The impact of the missing baselines can be very important and may easily be underestimated, or even overlooked. The present study uses ALMA archival data of the ²⁹SiO(8-7) line emission of the AGB star W Hydrae for a demonstration. A critical discussion of the reliability of the observations away from the star is presented together with comments of a broader scope. Properties of the circumstellar envelope of W Hya within ~15 au from the star, many of which are not mentioned in the published literature, are briefly described and compared with R Doradus, an AGB star having properties very similar to W Hya.

• Journal of Radiation Protection and Research
• /
• 제44권3호
• /
• pp.97-102
• /
• 2019

Background: Dose rate meters are the most widely used, and perhaps one of the most important tools for the measurement of ionising radiation. They are often the first, or only, device available to a user for an instant check of radiation dose at a certain location. Throughout the world, radiation safety practices rely strongly on the output of these dose rate meters. But how well do we know the quality of their output? Materials and Methods: This review is based on the measurements 1,158 commercially available dose rate meters of 116 different makes and models. Expected versus the displayed dose patterns and consistency was checked at various dose rates between $5{\mu}Gy{\cdot}h^{-1}$ and $2mGy{\cdot}h^{-1}$. Samples of these meters were then selected for further investigation and were exposed to radiation sources covering photon energies from 50 keV to 1.5 MeV. The effect of detector orientation on its reading was also investigated. Rather than focusing on the angular response distribution that is often reported by the manufacturer of the device, this study focussed on the design ergonomics i.e. the angles that the operator will realistically use to measure a dose rate. Results and Discussion: This review shows the scope and boundaries of the ionising radiation dose rate estimations that are made using commonly available meters. Observations showed both inter and intra make and model variations, occasional cases of instrument failure, instrument walk away, and erroneous response. Conclusion: The results indicate the significance of selecting and maintaining suitable monitors for specific applications in radiation safety.