• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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• pp.184-184
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• 2012

Recently, InGaN/GaN multi-quantum well grown on GaN pyramid structures have attracted much attention due to their hybrid characteristics of quantum well, quantum wire, and quantum dot. This gives us broad band emission which will be useful for phosphor-free white light emitting diode. On the other hand, by using quantum dot emission on top of the pyramid, site selective single photon source could be realized. However, these structures still have several limitations for the single photon source. For instance, the quantum efficiency of quantum dot emission should be improved further. As detection systems have limited numerical aperture, collection efficiency is also important issue. It has been known that micro-cavities can be utilized to modify the radiative decay rate and to control the radiation pattern of quantum dot. Researchers have also been interested in nano-cavities using localized surface plasmon. Although the plasmonic cavities have small quality factor due to high loss of metal, it could have small mode volume because plasmonic wavelength is much smaller than the wavelength in the dielectric cavities. In this work, we used localized surface plasmon to improve efficiency of InGaN qunatum dot as a single photon emitter. We could easily get the localized surface plasmon mode after deposit the metal thin film because lnGaN/GaN multi quantum well has the pyramidal geometry. With numerical simulation (i.e., Finite Difference Time Domain method), we observed highly enhanced decay rate and modified radiation pattern. To confirm these localized surface plasmon effect experimentally, we deposited metal thin films on InGaN/GaN pyramid structures using e-beam deposition. Then, photoluminescence and time-resolved photoluminescence were carried out to measure the improvement of radiative decay rate (Purcell factor). By carrying out cathodoluminescence (CL) experiments, spatial-resolved CL images could also be obtained. As we mentioned before, collection efficiency is also important issue to make an efficient single photon emitter. To confirm the radiation pattern of quantum dot, Fourier optics system was used to capture the angular property of emission. We believe that highly focused localized surface plasmon around site-selective InGaN quantum dot could be a feasible single photon emitter.

• 대한화학회지
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• 제63권6호
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• pp.453-458
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• 2019

Synthesis of ZnCo₂O₃ oxide is performed by sol-gel method via nitrate-citrate route. Powder X-ray diffraction (XRD) study shows monoclinic unit cell having lattice parameters: a = 5.721(1) Å, b = 8.073(2) Å, c = 5.670(1) Å, β = 93.221(8)°, space group P_2/m and Z = 4. Average crystallite sizes determined by Scherrer equation are the range ~14-32 nm, whereas SEM micrographs show nano-micro meter size particles formed in ZnCo₂O₃. Endothermic peak at ~798 K in the Differential scanning calorimetric (DSC) trace without weight loss could be due to structural transformation and the endothermic peak ~1143 K with weight loss is due to reversible loss of O₂ in air atmosphere. Energy Dispersive X-ray (EDX) analysis profile shows the presence of elements Zn, Co and O which indicates the purity of the sample. Magnetic measurements in the range of +12 kOe to -12 kOe at 10 K, 77 K, 120 K and at 300 K by PPMS-II Physical Property Measurement System (PPMS) shows hysteresis loops having very low values of the coercivity and retentivity which indicates the weakly ferromagnetic nature of the oxide. Observed X-band EPR isotropic lineshapes at 300 K and 77 K show positive g-shift at g_iso ~2.230 and g_iso ~2.217, respectively which is in agreement with the presence of paramagnetic site Co²⁺(3d⁷) in the oxide. DC conductivity value of 2.875 ×10^-8 S/cm indicates very weakly semiconducting nature of ZnCo₂O₃ at 300 K. DRS absorption bands ~357 nm, ~572 nm, ~619 nm and ~654 nm are due to the d-d transitions ⁴T_1g(⁴F)→²E_g(²G), ⁴T_1g(⁴F)→⁴T_1g(⁴P), ⁴T_1g(⁴F)→⁴A_2g(⁴F), ⁴T_1g(⁴F)→⁴T_2g(⁴F), respectively in octahedral ligand field around Co²⁺ ions. Direct band gap energy, E_g~ 1.5 eV in the oxide is obtained by extrapolating the linear part of the Tauc plot to the energy axis indicates fairly strong semiconducting nature of ZnCo₂O₃.

• 대한화학회지
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• 제46권1호
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• pp.7-13
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• 2002

자화수가 특이한 물리화학적 성질을 갖고 있음은 여러 학자들에 의하여 꾸준히 연구되어 왔는데, 아직도 자화수의 특성이 명확하게 설명되지 못하고 있는 실정이다. 본 연구에서는 자화수가 염류들의 침전반응 및 석고의 가수 경화반응에 미치는 영향을 다음과 같이 관찰하였다. $25^{\circ}C$ 항온조 내부에서 실시한 salt filter assay 방법으로 침전반응을 조사하였으며, $20^{\circ}C$ 실온에서 석고의 가수 경화반응 시간을 Gillmore needle의 방법으로 측정함으로써 석고의 가수 경화 속도를 조사하였다. 0.1M 염 이온들을 반응시킨 염류의 침전 반응 결과, $BaSO_4,\;BaCO_3,\;CaCO_3$의 침전 생성물의 양은 대조군의 증류수에 비하여 자화수에서 각각 약 3.6%, 3.8%, 4.4% 씩 증가되었으며, 석고의 최종 경화시간은 대조군의 증류수에 비하여 자화수에서 현저하게 감소되었으므로 자화수가 석고의 가수 경화속도를 촉진시키는 것으로 나타났다. 이는 대조군의 증류수에 비하여 자화수는 물분자가 치밀하게 구조화되어서 수많은 cluster들을 형성함으로서 물분자 사이의 결합 및 반응력이 증가되며, $Ba^{2+}$ 또는 $Ca^{2+}$ 같은 염류들에 대하여 특징적으로 반응해 침전반응 속도와 가수 경화 반응 속도가 증가된 것으로 추측된다.

• 한국산학기술학회논문지
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• 제19권8호
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• pp.14-18
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• 2018

일반적으로 반도체소자의 이동도를 높이기 위하여 반도체소자에서 옴접촉이 중요하게 다루어진다. 반도체 구조의 PN접합은 공핍층을 포함하고 있으며, 공핍층은 전기적인 비선형을 유도하고 쇼키접압을 만들어내는 반도체 고유의 물리적인 특징이다. 본 연구에서는 절연막이 전도성에 미치는 효과를 조사하기 위해서 $SiO_2$ 박막과 $V_2O_5/SiO_2$ 박막의 전기적인 특성을 비교하여 조사하였다. 미소전계영역에서 $SiO_2$ 절연막의 전기적인 특성으로부터 비선형 쇼키접합을 이루고 있는 것을 확인하였으며, 그 위에 증착된 $V_2O_5$ 박막은 오믹특성을 갖는 것을 확인하였다. 절연막의 PN 접합에 의한 쇼키접합 특성이 누설전류를 차단하여 $V_2O_5$ 박막의 전도성을 우수하게 만들었다. 양의 전압에서 $SiO_2$ 박막의 커패시턴스 값은 매우 낮았으나 $V_2O_5$ 박막의 커패시턴스 값은 전압이 증가할수록 증가하였다. 일반적인 전계영역에서 $SiO_2$ 박막의 절연 효과에 의해 $V_2O_5$ 박막의 전도성이 증가하는 것을 확인하였다. 절연박막은 공핍층의 효과를 이용하는 쇼키접합을 갖게 되며, 반도체에서의 쇼키접합은 전도성을 높이는 효과가 있는 것을 확인하였다.

• 한국분말재료학회지
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• 제9권6호
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• pp.394-408
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• 2002

Nanostructured high strength metastable Al-, Mg- and Ti-based alloys containing different amorphous, quasicrystalline and nanocrystalline phases are synthesized by non-equilibrium processing techniques. Such alloys can be prepared by quenching from the melt or by powder metallurgy techniques. This paper focuses on one hand on mechanically alloyed and ball milled powders containing different volume fractions of amorphous or nano-(quasi)crystalline phases, consolidated bulk specimens and, on the other hand. on cast specimens containing different constituent phases with different length-scale. As one example. $Mg_{55}Y_{15}Cu_{30}$- based metallic glass matrix composites are produced by mechanical alloying of elemental powder mixtures containing up to 30 vol.% $Y_2O_3$ particles. The comparison with the particle-free metallic glass reveals that the nanosized second phase oxide particles do not significantly affect the glass-forming ability upon mechanical alloying despite some limited particle dissolution. A supercooled liquid region with an extension of about 50 K can be maintained in the presence of the oxides. The distinct viscosity decrease in the supercooled liquid regime allows to consolidate the powders into bulk samples by uniaxial hot pressing. The $Y_2O_3$ additions increase the mechanical strength of the composites compared to the $Mg_{55}Y_{15}Cu_{30}$ metallic glass. The second example deals with Al-Mn-Ce and Al-Cu-Fe composites with quasicrystalline particles as reinforcements, which are prepared by quenching from the melt and by powder metallurgy. $Al_{98-x}Mn_xCe_2$ (x =5,6,7) melt-spun ribbons containing a major quasicrystalline phase coexisting with an Al-matrix on a nanometer scale are pulverized by ball milling. The powders are consolidated by hot extrusion. Grain growth during consolidation causes the formation of a micrometer-scale microstructure. Mechanical alloying of $Al_{63}Cu_{25}Fe_{12}$ leads to single-phase quasicrystalline powders. which are blended with different volume fractions of pure Al-powder and hot extruded forming $Al_{100-x}$$(Al_{0.63}Cu_{0.25}Fe_{0.12})_x$ (x = 40,50,60,80) micrometer-scale composites. Compression test data reveal a high yield strength of ${\sigma}_y{\geq}$700 MPa and a ductility of ${\varepsilon}_{pl}{\geq}$5% for than the Al-Mn-Ce bulk samples. The strength level of the Al-Cu-Fe alloys is ${\sigma}_y{\leq}$550 MPa significantly lower. By the addition of different amounts of aluminum, the mechanical properties can be tuned to a wide range. Finally, a bulk metallic glass-forming Ti-Cu-Ni-Sn alloy with in situ formed composite microstructure prepared by both centrifugal and injection casting presents more than 6% plastic strain under compressive stress at room temperature. The in situ formed composite contains dendritic hcp Ti solid solution precipitates and a few $Ti_3Sn,\;{\beta}$-(Cu, Sn) grains dispersed in a glassy matrix. The composite micro- structure can avoid the development of the highly localized shear bands typical for the room temperature defor-mation of monolithic glasses. Instead, widely developed shear bands with evident protuberance are observed. resulting in significant yielding and homogeneous plastic deformation over the entire sample.

• 한국표면공학회지
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• 제46권2호
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• pp.68-74
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• 2013

For the coating of diamond films on WC-Co tools, a buffer interlayer is needed because Co catalyzes diamond into graphite. W and Ti were chosen as candidate interlayer materials to prevent the diffusion of Co during diamond deposition. W or Ti interlayer of $1{\mu}m$ thickness was deposited on WC-Co substrate under Ar in a DC magnetron sputter. After seeding treatment of the interlayer-deposited specimens in an ultrasonic bath containing nanometer diamond powders, $2{\mu}m$ thick nanocrystalline diamond (NCD) films were deposited at $600^{\circ}C$ over the metal layers in a 2.45 GHz microwave plasma CVD system. The cross-sectional morphology of films was observed by FESEM. X-ray diffraction and visual Raman spectroscopy were used to confirm the NCD crystal structure. Micro hardness was measured by nano-indenter. The coefficient of friction (COF) was measured by tribology test using ball on disk method. After tribology test, wear tracks were examined by optical microscope and alpha step profiler. Rockwell C indentation test was performed to characterize the adhesion between films and substrate. Ti and W were found good interlayer materials to act as Co diffusion barriers and diamond nucleation layers. The COFs on NCD films with W or Ti interlayer were measured as less than 0.1 whereas that on bare WC-Co was 0.6~1.0. However, W interlayer exhibited better results than Ti in terms of the adhesion to WC-Co substrate and to NCD film. This result is believed to be due to smaller difference in the coefficients of thermal expansion of the related films in the case of W interlayer than Ti one. By varying the thickness of W interlayer as 1, 2, and $4{\mu}m$ with a fixed $2{\mu}m$ thick NCD film, no difference in COF and wear behavior but a significant change in adhesion was observed. It was shown that the thicker the interlayer, the stronger the adhesion. It is suggested that thicker W interlayer is more effective in relieving the residual stress of NCD film during cooling after deposition and results in stronger adhesion.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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• pp.241-241
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• 2008

Macrofore formation in silicon and other semiconductors using electrochemical etching processes has been, in the last years, a subject of great attention of both theory and practice. Its first reason of concern is new areas of macropore silicone applications arising from microelectromechanical systems processing (MEMS), membrane techniques, solar cells, sensors, photonic crystals, and new technologies like a silicon-on-nothing (SON) technology. Its formation mechanism with a rich variety of controllable microstructures and their many potential applications have been studied extensively recently. Porous silicon is formed by anodic etching of crystalline silicon in hydrofluoric acid. During the etching process holes are required to enable the dissolution of the silicon anode. For p-type silicon, holes are the majority charge carriers, therefore porous silicon can be formed under the action of a positive bias on the silicon anode. For n-type silicon, holes to dissolve silicon is supplied by illuminating n-type silicon with above-band-gap light which allows sufficient generation of holes. To make a desired three-dimensional nano- or micro-structures, pre-structuring the masked surface in KOH solution to form a periodic array of etch pits before electrochemical etching. Due to enhanced electric field, the holes are efficiently collected at the pore tips for etching. The depletion of holes in the space charge region prevents silicon dissolution at the sidewalls, enabling anisotropic etching for the trenches. This is correct theoretical explanation for n-type Si etching. However, there are a few experimental repors in p-type silicon, while a number of theoretical models have been worked out to explain experimental dependence observed. To perform ordered macrofore formaion for p-type silicon, various kinds of mask patterns to make initial KOH etch pits were used. In order to understand the roles played by the kinds of etching solution in the formation of pillar arrays, we have undertaken a systematic study of the solvent effects in mixtures of HF, N-dimethylformamide (DMF), iso-propanol, and mixtures of HF with water on the macrofore structure formation on monocrystalline p-type silicon with a resistivity varying between 10 ~ 0.01 $\Omega$ cm. The etching solution including the iso-propanol produced a best three dimensional pillar structures. The experimental results are discussed on the base of Lehmann's comprehensive model based on SCR width.

• 한국해양학회지:바다
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• 제13권4호
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• pp.333-341
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• 2008

청계만에는 3개의 방조제(창포, 복길, 구일)가 위치하고 있고 이로부터 유입되는 담수로 인한 환경의 변화가 예상된다. 이를 조사하기 위해 2006년 11월(가을), 2007년 2월(겨울), 5월(봄), 8월(여름)에 각 방조제 앞에서 3개 정점을 선정하였다. 각 방조제 정점에서 대발생은 갈수기인 2007년 2월에 대형식물플랑크톤에 의해 발생하였고 풍수기에는 중 형식물플랑크톤이 우점하는 분포를 나타냈다. 각 방조제 정점에서 풍수기에는 담수의 유입으로 인하여 염분과 투명도는 낮고 암모늄과 인산염은 갈수기인 2007년 2월보다 높게 나타났지만 식물플랑크톤 생체량은 낮게 나타났는데 이는 담수의 유입으로 인한 높은 탁도나 염분의 급격한 감소가 영양염류보다 더 영향을 미치는 것으로 사료된다. 즉 본 조사해역에서 갈수기인 2007년 2월에는 식물플랑크톤의 성장에 영양염류가 영향을 미치지만 풍수기에는 높은 탁도나 급격한 염분변화가 영양염류보다 더 큰 영향을 미치는 것으로 판단된다.

• 한국해양학회지:바다
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• 제21권1호
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• pp.24-35
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• 2016

2014년 울산만 내, 외측 해역에서 해양환경의 계절 변화가 식물플랑크톤 군집의 공간 분포에 미치는 영향을 파악하였다. 울산만을 태화강 하구에 위치한 내측과 외양 영향을 강하게 받는 외측으로 나누어, 내측과 외측의 환경 차이를 t-test로 검증하였다. 수온은 동계(t = -5.833, p < 0.01)와 추계(p > 0.05)에는 외측이 높았고, 춘계(t = 4.247, p < 0.01)와 하계(t = 2.876, p < 0.05)에는 내측이 높았다. 염분은 추계를 제외한 모든 계절에 내측에서 외측보다 유의하게 낮았다(p < 0.01). 동계에는 수층 혼합에 의해 전 수층에서 영양염 농도가 높았고, 하계에는 담수 유입으로 내측 표층에서 현저하게 높았다. 크기 분획된 Chl. a 양은 $20{\mu}m$보다 작은 크기의 nano, pico식물플랑크톤의 양이 많았다. 극미소 식물플랑크톤은 영양염 농도가 낮은 외양 환경에서 적응력이 높은데 이러한 결과는 조사해역이 외양의 영향을 강하게 받고 있음을 시사한다. 춘계와 하계에는 내측 정점을 중심으로 유글레나류 Eutreptiella gymnastica의 밀도가 특이적으로 높았다. 이는 강우 후 많은 담수가 유입되어 저염분 환경이 조성되고 DIN (nitrate+nitrite, ammonium)이 대량 공급되었기 때문이다. 하계에는 태화강으로부터 다량의 담수가 공급되어 담수미세 남조류 Oscillatoria sp., Microcystis sp.가 내측 정점(1-5)을 중심으로 높은 밀도로 출현하였다. 추계와 동계에는 규조류와 은편모류가 우점하였다. 높은 현존량을 보인 중심 규조류Chaetoceros 속은 성층 약화로 저층에서 공급되는 영양염류의 영향을 받아 빠르게 성장하였고, 은편모조류는 다른 식물플랑크톤의 상대적인 성장 둔화로 기회적으로 우점하였다. 결과적으로 울산만은 강우기인 춘계와 하계에 태화강의 영향을 강하게 받아 내측 정점을 중심으로 저염분, 고영양염 환경이 유지되었고, 추계와 동계에는 만 외측 외양수의 영향을 크게 받았으며, 식물플랑크톤 군집은 크게 이 두가지 환경요인에 의해 계절적으로 제어되는 것으로 판단되었다.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2011년도 제36회 춘계학술대회논문집
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• pp.1-2
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• 2011

Hybrid rockets have lately attracted attention as a strong candidate of small, low cost, safe and reliable launch vehicles. A significant topic is that the first commercially sponsored space ship, SpaceShipOne vehicle chose a hybrid rocket. The main factors for the choice were safety of operation, system cost, quick turnaround, and thrust termination. In Japan, five universities including Hokkaido University and three private companies organized "Hybrid Rocket Research Group" from 1998 to 2002. Their main purpose was to downsize the cost and scale of rocket experiments. In 2002, UNISEC (University Space Engineering Consortium) and HASTIC (Hokkaido Aerospace Science and Technology Incubation Center) took over the educational and R&D rocket activities respectively and the research group dissolved. In 2008, JAXA/ISAS and eleven universities formed "Hybrid Rocket Research Working Group" as a subcommittee of the Steering Committee for Space Engineering in ISAS. Their goal is to demonstrate technical feasibility of lowcost and high frequency launches of nano/micro satellites into sun-synchronous orbits. Hybrid rockets use a combination of solid and liquid propellants. Usually the fuel is in a solid phase. A serious problem of hybrid rockets is the low regression rate of the solid fuel. In single port hybrids the low regression rate below 1 mm/s causes large L/D exceeding a hundred and small fuel loading ratio falling below 0.3. Multi-port hybrids are a typical solution to solve this problem. However, this solution is not the mainstream in Japan. Another approach is to use high regression rate fuels. For example, a fuel regression rate of 4 mm/s decreases L/D to around 10 and increases the loading ratio to around 0.75. Liquefying fuels such as paraffins are strong candidates for high regression fuels and subject of active research in Japan too. Nakagawa et al. in Tokai University employed EVA (Ethylene Vinyl Acetate) to modify viscosity of paraffin based fuels and investigated the effect of viscosity on regression rates. Wada et al. in Akita University employed LTP (Low melting ThermoPlastic) as another candidate of liquefying fuels and demonstrated high regression rates comparable to paraffin fuels. Hori et al. in JAXA/ISAS employed glycidylazide-poly(ethylene glycol) (GAP-PEG) copolymers as high regression rate fuels and modified the combustion characteristics by changing the PEG mixing ratio. Regression rate improvement by changing internal ballistics is another stream of research. The author proposed a new fuel configuration named "CAMUI" in 1998. CAMUI comes from an abbreviation of "cascaded multistage impinging-jet" meaning the distinctive flow field. A CAMUI type fuel grain consists of several cylindrical fuel blocks with two ports in axial direction. The port alignment shifts 90 degrees with each other to make jets out of ports impinge on the upstream end face of the downstream fuel block, resulting in intense heat transfer to the fuel. Yuasa et al. in Tokyo Metropolitan University employed swirling injection method and improved regression rates more than three times higher. However, regression rate distribution along the axis is not uniform due to the decay of the swirl strength. Aso et al. in Kyushu University employed multi-swirl injection to solve this problem. Combinations of swirling injection and paraffin based fuel have been tried and some results show very high regression rates exceeding ten times of conventional one. High fuel regression rates by new fuel, new internal ballistics, or combination of them require faster fuel-oxidizer mixing to maintain combustion efficiency. Nakagawa et al. succeeded to improve combustion efficiency of a paraffin-based fuel from 77% to 96% by a baffle plate. Another effective approach some researchers are trying is to use an aft-chamber to increase residence time. Better understanding of the new flow fields is necessary to reveal basic mechanisms of regression enhancement. Yuasa et al. visualized the combustion field in a swirling injection type motor. Nakagawa et al. observed boundary layer combustion of wax-based fuels. To understand detailed flow structures in swirling flow type hybrids, Sawada et al. (Tohoku Univ.), Teramoto et al. (Univ. of Tokyo), Shimada et al. (ISAS), and Tsuboi et al. (Kyushu Inst. Tech.) are trying to simulate the flow field numerically. Main challenges are turbulent reaction, stiffness due to low Mach number flow, fuel regression model, and other non-steady phenomena. Oshima et al. in Hokkaido University simulated CAMUI type flow fields and discussed correspondence relation between regression distribution of a burning surface and the vortex structure over the surface.