• 한국광학회지
• /
• 제1권1호
• /
• pp.7-11
• /
• 1990

수은 원자 증기에 강한 레이저 광$(10-120GW/\textrm{cm}^2)$을 조사하여 수은 원자의 공명 다광자 이온화 과정을 연구하였다. 파장 560.7nm의 광자 4개를 흡수할 때 공명준위는 $6d ^1D_2$이다. 수은 증기압(0.1-3.0 Torr)과 레이저 파장(559-569nm)을 변화시키면서 큰 강도의 광원과 원자가 상호작용하여 생기는 AC Stark 이동과 line broadening의 변화를 조사하였고, 원자 밀도의 증가에 따라 이온화율의 증가가 둔화되다가 감소되는 것도 관측되었다. 이동계수 $\alpha$=0.6cm-1/GW/$\textrm{cm}^2$로 측정되었다. 특히, 이온화율의 레이저 강도 의존성을 나타내는 비선형 차수를 공명파장에서 측정한 결과 k=3을 얻었으며, 이론적인 결과와 비교하였다.

• 대한기계학회:학술대회논문집
• /
• 대한기계학회 2004년도 추계학술대회
• /
• pp.1213-1218
• /
• 2004

The present article reports extensive numerical results on the non-local characteristics of ultra-short pulsed laser-induced breakdowns of fused silica ($SiO_{2}$) by using the multivariate Fokker-Planck equation. The nonlocal type of multivariate Fokker-Planck equation is modeled on the basis of the Boltzmann transport formalism to describe the ultra-short pulsed laser-induced damage phenomena in the energy-position space, together with avalanche ionization, three-body recombination, and multiphoton ionization. Effects of electron avalanche, recombination, and multiphoton ionization on the electronic transport are examined. From the results, it is observed that the recombination becomes prominent and contributes to reduce substantially the rate of increase in electron number density when the electron density exceeds a certain threshold. With very intense laser irradiation, a strong absorption of laser energy takes place and an initially transparent solid is converted to a metallic state, well known as laser-induced breakdown. It is also found that full ionization is provided at intensities above threshold, all further laser energy is deposited within a thin skin depth.

• Bulletin of the Korean Chemical Society
• /
• 제34권3호
• /
• pp.907-911
• /
• 2013

Numbers of matrix- and analyte-derived ions and their sum in matrix-assisted laser desorption ionization (MALDI) of a peptide were measured using 2,5-dihydroxybenzoic acid (DHB) as matrix. As for MALDI with ${\alpha}$-cyano-4-hydroxy cinnamic acid as matrix, the sum was independent of the peptide concentration in the solid sample, or was the same as that of pure DHB. This suggested that the matrix ion was the primary ion and that the peptide ion was generated by matrix-to-peptide proton transfer. Experimental ionization efficiencies of $10^{-5}-10^{-4}$ for peptides and $10^{-8}-10^{-7}$ for matrices are far smaller than $10^{-3}-10^{-1}$ for peptides and $10^{-5}-10^{-3}$ for matrices speculated by Hillenkamp and Karas. Number of gas-phase ions generated by MALDI was unaffected by laser wavelength or pulse energy. This suggests that the main role of photo-absorption in MALDI is not in generating ions via a multi-photon process but in ablating materials in a solid sample to the gas phase.

• 한국의학물리학회지:의학물리
• /
• 제32권4호
• /
• pp.137-144
• /
• 2021

Purpose: This study aimed to investigate the accuracy of head scatter factor (S_c) by applying a developed multi-leaf collimator (MLC) scatter source model for an unflattened photon beam. Methods: Sets of S_c values were measured for various jaw-defined square and rectangular fields and MLC-defined square fields for developing dual-source model (DSM) and MLC scatter model. A 6 MV unflattened photon beam has been used. Measurements were performed using a 0.125 cm³ cylindrical ionization chamber and a mini phantom. Then, the parameters of both models have been optimized, and S_c has been calculated. The DSM and MLC scatter models have been verified by comparing the calculated values to the three S_c set measurement values of the jaw-defined field and the two S_c set measurement values of MLC-defined fields used in the existing modeling, respectively. Results: For jaw-defined fields, the calculated S_c using the DSM was consistent with the measured S_c value. This demonstrates that the DSM was properly optimized and modeled for the measured values. For the MLC-defined fields, the accuracy between the calculated and measured S_c values with the addition of the MLC scatter source appeared to be high, but the only use of the DSM resulted in a significantly bigger differences. Conclusions: Both the DSM and MLC models could also be applied to an unflattened beam. When considering scattered radiation from the MLC by adding an MLC scatter source model, it showed a higher degree of agreement with the actual measured S_c value than when using only DSM in the same way as in previous studies.

• 대한기계학회논문집B
• /
• 제29권4호
• /
• pp.453-459
• /
• 2005

In this paper, we are proposing a robust tool which is capable of measuring the size and elemental composition of submicron particles from twenty to several hundreds nanometers at the same time, i.e., named Single Particle Mass Spectrometer (SPMS). The home-made SPMS employs a laser ablation/multi-photon ionization method to tear a nanoparticle into the constituent elemental ions. One thing different from the conventional Aerosol Time-of-Flight Mass Spectrometer (ATOFMS) is the power of the ionization laser. Much strong laser used in this work makes it possible to generate elemental ions rather than molecular ions from a nanoparticle. Also the use of high power laser may guarantee a complete ionization of a particle, which was confirmed by the existence of multiple charged ions. If a particle is evaporated/ionized completely and detected through electric field-free TOF tube without any loss, we can extract the original particle volume from the measured total ion numbers. Collecting a number of particles mass spectra, we get a database of size and elemental composition of nanoparticles, with which we may take a took into any kinds of chemical reaction occurring at nanoscale. Several issues related to size estimation by SPMS will be discussed.

• 천문학회보
• /
• 제44권1호
• /
• pp.75.1-75.1
• /
• 2019

The universe has been ionized in the post-reionization by several photon contributors. The dominant source to produce the hydrogen ionizing photons is not revealed so far. Faint quasars have been expected to generate UV photon budgets required to maintain ionization state of universe. Observational limits, however, hinder to discover them despite their higher number density than bright one. Consequently, the influence of faint quasars on post-reionization are not considered sufficiently. Therefore, a survey to find faint quasars at z ~ 5 is crucial to determine the main ionizing source in the post-reionization era. Deep images from the Hyper Suprime-Cam Subaru Strategic Program (HSC SSP) allow us to search for quasar swith low luminosities in the ELAIS-N1 field. J band information are obtained by the Infrared Medium-deep Survey (IMS) and the UKIRT Infrared Deep Sky Survey (UKIDSS) - Deep ExtragalacticSurvey (DXS). Faint quasar candidates were selected from several multi-band color cut criteria based on simulated quasars on color-color diagram. To choose the reliable candidates with possible Lyman break, we have performed medium-bands observations. Whether a candidate is a quasar or a dwarf star contamination was decided by results from chi-square minimization of quasar/dwarf model fitting. Spectroscopic follow-up observations confirm three quasars at z ~ 5. 100% spectral confirmation success rate implies that the medium-band observations effectively select faint quasars with strong Lyman alpha emission.

• 한국의학물리학회지:의학물리
• /
• 제16권3호
• /
• pp.111-115
• /
• 2005

본 연구에서는 치료용 광자선의 품질관리를 위하여 다채널 측정기를 개발하였다. 측정기는 여러 개의 전리함들이 삽입된 팬텀으로 구성되어 있다. 각 전리함은 탄소가 도포된 마이크로필름으로 제작된 초소형 평행평판 전리함과 같다. 본 연구에서는 고체 팬텀에 삽입된 6개의 전리함에 대하여 6 MV X-선을 이용하여 전기적 특성을 조사하였다 측정결과 누설전류는 0.5 ph 이내로 안정적이었고, 재현성은 0.5$\%$, 선형성은 0.5$\%$ 이내로 나타났다. 그리고 선량률 효과는 모든 전리함이 0.7$\%$ 이하로 나타났다. 또한 다른 전리함의 영향으로 인한 흡수선량의 변화는 약 0.8$\%$ 이내로 나타났다. 개발된 측정기는 치료용 광자선에 대하여 출력측정 시 선질결정에 활용할 수 있으며 근사적인 깊이선량률의 측정에도 이용될 수 있다.

• 한국의학물리학회지:의학물리
• /
• 제11권2호
• /
• pp.147-155
• /
• 2000

Patient dose verification is one of the most important parts in quality assurance of the treatment delivery for radiation therapy. The dose distributions may be meaningfully improved by modulating two dimensional intensity profile of the individual high energy radiation beams In this study, a new method is presented for the pre-treatment dosimetric verification of these two dimensional distributions of beam intensity by means of a charge coupled device video camera-based fluoroscopic device (henceforth called as CCD-VCFD) as a radiation detecter with a custom-made software for dose calculation from fluorescence signals. This system of dosimeter (CCD-VCFD) could reproduce three dimensional (3D) relative dose distribution from the digitized fluoroscopic signals for small (1.0$\times$1.0 cm$^2$ square, ø 1.0 cm circular ) and large (30$\times$30cm$^2$) field sizes used in intensity modulated radiation therapy (IMRT). For the small beam sizes of photon and electron, the calculations are performed In absolute beam fluence profiles which are usually used for calculation of the patient dose distribution. The good linearity with respect to the absorbed dose, independence of dose rate, and three dimensional profiles of small beams using the CCD-VCFD were demonstrated by relative measurements in high energy Photon (15 MV) and electron (9 MeV) beams. These measurements of beam profiles with CCD-VCFD show good agreement with those with other dosimeters such as utramicro-cylindrical (UC) ionization chamber and radiographic film. The study of the radiation dosimetric technique using CCD-VCFD may provide a fast and accurate pre-treatment verification tool for the small beam used in stereotactic radiosurgery (SRS) and can be used for verification of dose distribution from dynamic multi-leaf collimation system (DMLC).

• Radiation Oncology Journal
• /
• 제15권1호
• /
• pp.71-78
• /
• 1997

목적 :동적 쐐기 조사면 측정을 다중 검출기 시스템과 같은 특수한 장치없이 보편적인 방사선 측정 방법을 사용하여 시행할 수 있는 방법을 고안, 수행하였다. 대상 및 방법 : $15^{\circ},\;30^{\circ},\;45^{\circ},\;60^{\circ}$의 동적 쐐기각(dynamic wedge angle)과 6MV와 15MV인 광자선을 발생시키는 선형 가속기(CL 2100 C/D)를 이용하여 wedge transmission factor 및 percentage depth dose(PDD, 선량 프로파일을 측정하였다. Wedge transmission factor는 6MV, 15MV인 광자선과 $15^{\circ},\;30^{\circ},\;45^{\circ},\;60^{\circ}$의 4개의 동적 쐐기각에 대해서 $4\times4cm^2-20\times20cm^2$까지 1-2cm간격의 정사각형 조사면과 Y-field가 4cm, 20cm일 때 여러개의 X-field에 대한 각각의 직사각형 조사면에서 측정하였다. 또한 동적 쐐기의 구간별 치료표(Segmented Treatment Table, STT)값을 이용하여 wedge factor를 계산해 내었다. PDD는 필름 dosimetry로 구하였는데 개방 조사면에 대해 전리함과 필름으로 PDD를 구한 후 필름의 환산값을 알아내어 쐐기 조사면에 대한 필름 dosimetry로 PDD를 구하여 필름 환산값으로 전리함을 통해 얻을 수 있는 실제 PDD를 구하였다. 선량 프로파일은 비대칭 정지 조사면을 선택적으로 전리함을 이용하여 측정하고 이때 얻은 측정치인 소구간 프로파일과 STT를 이용하는 선량 분포 중칩 방식으로 구하였다. 결과 : wedge transmission factor의 측정치와 STT를 이용하여 구한 계산치를 비교한 결과 실험 오차 범위내에서 거의 일치하였다. 또한 직사각형 조사면에서의 wedge transmission factor 변화를 측정한 결과 동일한 Y-field에 대해서 직사각형 조사면은 정사각형 조사면에서의 wedge factor와 같았다. PDD는 필름 방사선 측정값의 보정으로 개방 조사면에서 PDD와 동적 쐐기 조사면에서 PDD 사이의 차이는 무시될 수 있다. 그리고 전리함의 측정으로부터 중칩 방식으로 얻어진 동적 쫴기의 선량 프로파일은 필름 dosimetry로 얻은 동적 쐐기의 선량 프로파일과 비교한 결과 최대 2% 이내 정확도의 허용 오차 영역에 들어옴을 볼 수 있었다. 결론 :동적 조사면의 특성으로 동적 쐐기 측정에서의 정보 수집을 위하여 모든 조사면에서의 방대한 측정과 그로인한 장시간의 소비, 또한 동적 쐐기 측정을 위한 특수한 장치가 필요하지만 보편적으로 사용하는 측정 장치, 즉 단일 검출기와 필름 방사선 측정 방법으로 충분히 용이하게 행할 수 있었다.

• 대한방사선기술학회지:방사선기술과학
• /
• 제43권2호
• /
• pp.105-114
• /
• 2020

This study aimed to assess of beam-matching accuracy for an 8 MV beam between the same model linear accelerators(Linac) commissioned over two years. Two models were got the customer acceptance procedure(CAP) criteria. For commissioning data for beam-matched linacs, the percentage depth doses(PDDs), beam profiles, output factors, multi-leaf collimator(MLC) leaf transmission factors, and the dosimetric leaf gap(DLG) were compared. In addition, the accuracy of beam matching was verified at phantom and patient levels. At phantom level, the point doses specified in TG-53 and TG-119 were compared to evaluate the accuracy of beam modelling. At patient level, the dose volume histogram(DVH) parameters and the delivery accuracy are evaluated on volumetric modulated arc therapy(VMAT) plan for 40 patients that included 20 lung and 20 brain cases. Ionization depth curve and dose profiles obtained in CAP showed a good level for beam matching between both Linacs. The variations in commissioning beam data, such as PDDs, beam profiles, output factors, TF, and DLG were all less than 1%. For the treatment plans of brain tumor and lung cancer, the average and maximum differences in evaluated DVH parameters for the planning target volume(PTV) and the organs at risk(OARs) were within 0.30% and 1.30%. Furthermore, all gamma passing rates for both beam-matched Linacs were higher than 98% for the 2%/2 mm criteria and 99% for the 2%/3 mm criteria. The overall variations in the beam data, as well as tests at phantom and patient levels remains all within the tolerance (1% difference) of clinical acceptability between beam-matched Linacs. Thus, we found an excellent dosimetric agreement to 8 MV beam characteristics for the same model Linacs.