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Design and Implementation of NAREGI SuperScheduler Based on the OGSA Architecture

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Journal of Computer Science & Technology 2006年第4期21卷 521-528页

作者： Satoshi matsuoka Masayuki Hatanaka Yasumasa Nakano Yuji Iguchi Toshio Ohno Kazushige Saga Hidemoto Nakada Global Scientific Information and Computing Center Tokyo Institute of Technology 2-12-10okayama Meguro-ku Tokyo 152-8550 Japan Center for Grid Research and Development National Institute of Informatics 1-105 Kanda-Jinbocho Chiyoda-ku Tokyo 101-0051 Japan linux Software Development Div. Server Systems Unit. Fujitsu Limited 130 Miyamoto Numazu-shi Shizuoka410-0396 Japan Grid Technology Research Center National Institute of Advanced Industrial Science and Technology 1-18-13 Sotokanda Chiyoda-ku Tokyo 101-0021 Japan

NAREGI is a 5-year Japanese National Grid Project during 2003--2007, whose chief aim is to develop a set of grid middleware to serve as a basis for future e-Science. NAREGI also aims to lead the way in standardization of grid middleware, based on the OGSA architecture. Its super-scheduler is based on the proposed OGSA-EMS Architecture, in that it becomes the first working implementation that implements the documented component relationships within the OGSA-EMS architecture document v.l.0. Through the efforts and experience in the design and implementation, it has been confirmed that the documented OGSA-EMS architecture is quite feasible, but will require significant amount of refinement and speed improvements to finalize its detailed specifications. The super-scheduler also supports co-allocation across multiple sites to support automated execution of grid-based MPIs that execute across machines. Such a resource allocation requires sophisticated interactions between the OGSA-EMS components not covered in the current OGSA-EMS architecture, some of which are non-trivial. Overall, job scheduling with OGSA-EMS has proven to not only work, but also that its job allocation and execution time is within reasonable bounds.

关键词： grid scheduling resource management open grid services architecture OGSA

The Cyst Wall Formation during Encystment in the Ciliated Protozoa, Colpoda Cucullus

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The Cyst Wall Formation during Encystment in the Ciliated Pr...

Acoustic Absorption Characteristics of Perforated Thin Plate with Air Jets and Cavity

12th International Congress of Protozoology

作者： Akemi Kida Keisuke Yamamoto Tomoko Watoh Tatsuomi matsuoka Department of Biology Faculty of Science Kochi UniversityKochi 780-8520Japan Department of Biology Faculty of Science Kochi UniversityKochi 780-8520Japan Department of Biology Faculty of Science Kochi UniversityKochi 780-8520Japan Department of Biology Faculty of Science Kochi UniversityKochi 780-8520Japan

＜正＞Changes in the cell structure during encystment of Colpoda cucullus have been studied. In this study we were successful in observing the detail process of cyst wall formation by light and electron microscopy. Stage 1 （0-1.5 hr after encystment induction）: A number of small vesicles containing the electron-dense and toluidine blue （TB） positive materials appeared. The contents contained in the small vesicles were excreted into the large vacuoles which were opened to extracellular space. In the late stage 1, the precystic cells were rounded and surrounded by the first-synthesized cyst wall layer （l1 layer）. The cilia were resorbed inside of l1 layer. Stage 2 （1.5-5 hr）: Secondary layer （l2 layer） was formed and

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Open Journal of Fluid Dynamics 2015年第1期5卷 1-9页

作者： Hiromitsu Hamakawa Hiroki matsuoka Taiki Yamai Kenta Asakura Toru Otsuru Reiji Tomiku Eru Kurihara Hidechito Hayashi Eiichi Nishida Department of Mechanical Engineering Oita University Oita Japan Graduate School Master’s Program of Engineering Oita University Oita Japan Torishima Pump Mfg. Co. Ltd Takatsuki-shi Osaka Japan Department of Architecture Oita University Oita Japan Department of Mechanical Engineering Nagasaki University Nagasaki Japan Department of Mechanical Systems Engineering Shonan Institute of Technology Fujisawa-shi Kanagawa Japan

The present paper focuses on the effect of air jets through a perforated thin plate on the characteristics of an acoustic absorption coefficient. We measured the flow rate, internal pressure, acoustic pressure, and transfer function by using an improved acoustic impedance tube. The normal incidence absorption coefficient was calculated from the measured transfer function using transfer function methods. As a result, the frequency characteristics of the acoustic absorption coefficient against the frequency showed a maximum value at the local frequency. The peak frequency of the acoustic absorption coefficient depended on the thickness of the background air space and the thickness of the perforated plate. As the flow rate increased through the micropores, the peak level of the acoustic absorption coefficient also increased until a flow rate of 80?l /min. As the flow rate further increased, the peak level of the acoustic absorption coefficient decreased and that of the high frequency band increased.

关键词： Acoustic Absorption Coefficient Perforated Plate Cavity Micropores Air Jets Acoustic Impedance Tube

基于星载l波段SAR影像与地震烈度信息整合的建筑物破坏评估

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地壳构造与地壳应力 2010年第2期 1-12页

作者： Masashi matsuoka Nobuoto Nojima 安立强（翻译）罗毅（校对） Information Technology Research Institute National Institute of Advanced Industrial Science and TechnologySite 2 1-1-1 Umezono Tsukuba 305-8568 Japan Department of Civil Engineering Faculty of Engineering Gifu University I-1 Yanagido Gifu 501-1193 Japan 不详

为能在全世界范围快速稳定地评估地震建筑物破坏情况,文章应用装载于AlOS卫星上的l波段相控阵列合成孔径雷达(PAlSAR)提出了一个建筑物破坏估计模型,模型整合了星载SAR影像的应用与日本气象厅的分级地震烈度数据。为将现有的基于C波段SA... 详细信息

为能在全世界范围快速稳定地评估地震建筑物破坏情况,文章应用装载于AlOS卫星上的l波段相控阵列合成孔径雷达(PAlSAR)提出了一个建筑物破坏估计模型,模型整合了星载SAR影像的应用与日本气象厅的分级地震烈度数据。为将现有的基于C波段SAR影像的破坏评估模型发展成基于l波段SAR影像的模型,本文首先以1995年阪神地震的日本资源卫星1号(JERS-1)的l波段SAR影像数据以及真实细致的地面调查数据为基础,重新构建了严重破坏比率的似然函数。然后将整合了以地震烈度为自变量的脆性函数和本文提出的似然函数的模型应用于2007年秘鲁皮斯科地震受灾区域的PAlSAR影像。最后,通过与地面调查数据和高分辨率卫星影像的对比对破坏评估模型的准确程度进行检验。

关键词： SAR影像建筑物破坏地震烈度评估模型信息整合 l波段星载高分辨率卫星影像

合并胎儿水肿的肺叶外型肺隔离症患儿的静脉动脉化

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世界核心医学期刊文摘（儿科学分册） 2006年第8期2卷 48-49页

作者： Kitano Y. matsuoka K. Honna T. 贺莉 Division of General Surgery National Center for Child Health and DevelopmentSetagaya-kuTokyo 157-8535Japan

Background/Purpose:Fetal extralobar pulmonary sequestration(EPS)is sometime s complicated by massive pleural effusion(PE)leading to fetal *** und erlying mechanisms as well as the origin of the fluid are not well understood.T his study was performed to find a histological hallmark of an EPS with massive P *** hypothesized that venous obstruction has a role to play in the mechanisms of fluid production by ***:We recently experienced 3 cases of fetal EP S complicated by fetal hydrothoraxrequiring thoracentesis and eventually thoraco amniotic shunt *** protein content and cell count were measured in the aspirates,which were compared with chylothorax cases(n = 5)requiring feta l shunt *** birth,all 3 infants required mass resection for the co ntrol of *** venous wall thickness was measured on pathology slides stained with Elastica van Gieson *** of the media and adventitia was mea sured in approximately 40 veins per *** were corrected by external diamet er and expressed as percentage of medial thickness and percentage of adventitial *** EPS not associated with PE but with congenital diaphragmatic hern ia served as a ***:Total protein and the cell count of the EPS rel ated PE were 0.6 ±0.3 mg/dl and 28 ±14/μl(mean ±SD),which were significantly lower than those of PE i n chylothorax(2.2 ±0.2 mg/dl and 1900 ±1100/μl).Percentages of adventitial thickness of EPS with PE were 9.8%±3.8%,10.4%±3.6%,and 8.3%±3.7%,whi ch were significantly increased compared with the control of 3.1%±1.3%(P l thickness of EPS with PE were 7.0%±1.9%,7.3%±1.4%,and 6.6%±2.3%,which were significantly increased compared with the cont rol of 2.3%±0.7%(Plusions:We conclude that PE associated with EPS is the transudate rather than the *** thickened media and the adventi tia found in EPS with PE support the hypothesis that partial obstruction of the venous system leads to an i

关键词：肺叶外型肺隔离症静脉动脉化胎儿水肿患儿胸膜腔积液胸腔穿刺术先天性膈疝 EPS 静脉阻塞胸腔积液

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医源性肝外动脉假性动脉瘤处理及预后

中华肝胆外科杂志 2008年第2期14卷 104-104页

作者： Christensen T matsuoka l Heestand G 黄辉(摘) 邹一平(校) 不详解放军总医院第二附属医院北京100091

肝外动脉假性动脉瘤是手术以及创伤后相对不常见的损害。该报道中作者分析血管损害的表现、处理及预后。在相关外科过程中，报告发生率最高的为腹腔镜胆囊切除术（lC），作者分析相关文献并报告他们的经验。尤其突出肝外动脉假性动脉瘤... 详细信息

肝外动脉假性动脉瘤是手术以及创伤后相对不常见的损害。该报道中作者分析血管损害的表现、处理及预后。在相关外科过程中，报告发生率最高的为腹腔镜胆囊切除术（lC），作者分析相关文献并报告他们的经验。尤其突出肝外动脉假性动脉瘤与肝内假性动脉瘤相区分。作者总结了1995年9月至2004年7月间的6例病例，男女各3例，共7处假性动脉瘤。平均年龄67岁（48～80岁），行内镜、B超、CT、血管造影检查，给予线圈栓塞、动脉结扎和（或）肝切除治疗。结果示：假性动脉瘤平均大小4．9cm（1～11cm）；右肝动脉发生5例，胰十二指肠下动脉1例，胃十二指肠动脉1例；6例病人均有手术或穿刺过程。平均潜伏期（穿刺过程到处理）17周（1个月至16年）。

关键词：动脉假性动脉瘤肝外预后医源性腹腔镜胆囊切除术胃十二指肠动脉作者分析血管造影检查

Complex Regulation of Prolyl-4-Hydroxylases Impacts Root Hair Expansion

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Molecular Plant 2015年第5期8卷 734-746页

作者： Silvia M. Velasauez Martiniano M. Ricardi Christian Peter Poulsen Ai Oikawa Adiphol Dilokpimol Adnan Halim Silvina Mangano Silvina Paola Denita Juarez Eliana Marzol Juan D. Salgado Salter Javier Gloazzo Dorosz Cecilia Borassi Svenning Rune Moller Rafael Buono Yukiko Ohsawa Ken matsuoka Marisa S. Otegui Henrik V. Scheller Naomi Geshi Bent larsen Petersen Norberto D. lusem Jose M. Estevez Instituto de Fisiologfa Biologia Molecular y Neurociencias (IFIBYNE-CONICET) Facultad de Ciencias Exactas y Naturales Universidad de Buenos AiresBuenos Aires C1428EGA Argentina VKR Research Centre Department of Plant and Environmental Sciences University of Copenhagen DK-1871 Frededksberg C Denmark Joint BioEnergy Institute Feedstocks Division Lawrence Berkeley National Laboratory 5885 Hollis Street Emeryville CA 94608 USA Copenhagen Center for Glycomios Department of Cellular and Molecular Faculty of Health and Medical Sciences University of CopenhagenDK-2200 Copenhagen N Denmark Department of Botany University of Wisconsin Madison WI 53706 USA RIKEN Plant Science Center Tsurumi-ku Yokohama 230-0045 Japan laboratory of Plant Nutrition Faculty of Agriculture Kyushu University Hakozaki 6-10-1 Higashi-ku Fukuoka 812-8581 Japan Departamento de Fisiologia Biologia Molecular y Celular Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires Buenos Aires C1428EGAArgentina These authors contributed equally to the article. Present address: Fungal Physiology CBS-KNAW Fungal Biodiversity Center Uppsalalaan 8 Utrecht 3584 CT The Netherlands Present address: The Danish Stem Cell Center The Panum Institute Blegdamsvej 3B DK-2200 Copenhagen Denmark

Root hairs are single cells that develop by tip growth, a process shared with pollen tubes, axons, and fungal hyphae. However, structural plant cell walls impose constraints to accomplish tip growth. In addition to polysaccharides, plant cell walls are composed of hydroxyproline-rich glycoproteins （HRGPs）, which include several groups of O-glycoproteins, including extensins （EXTs）. Proline hydroxylation, an early post-translational modification （PTM） of HRGPs catalyzed by prolyl 4-hydroxylases （P4Hs）, defines their subsequent O-glycosylation sites. In this work, our genetic analyses prove that P4H5, and to a lesser extent P4H2 and P4H13, are pivotal for root hair tip growth. Second, we demonstrate that P4H5 has in vitro preferred specificity for EXT substrates rather than for other HRGPs. Third, by P4H promoter and protein swapping approaches, we show that P4H2 and P4H13 have interchangeable functions but cannot replace P4H5. These three P4Hs are shown to be targeted to the secretory pathway, where P4H5 forms dimers with P4H2 and P4H13. Finally, we explore the impact of deficient proline hydroxylation on the cell wall architec- ture. Taken together, our results support a model in which correct peptidyl-proline hydroxylation on EXTs, and possibly in other HRGPs, is required for proper cell wall self-assembly and hence root hair elongation in Arabidopsis thaliana.

关键词： enzymology cell expansion cell walls protein targeting proline hydroxylation root hairs

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超强激光脉冲与低密度泡沫靶相互作用研究

超强激光脉冲与低密度泡沫靶相互作用研究

Measurement of the integrated luminosity of the Phase 2 data of the Belle Ⅱ experiment

2004年全国强场激光物理会议

作者：李玉同盛政明张杰马燕云金展 Z．l．Chen R．Kodama T．matsuoka M．Tampo K．A．Tanaka T．Tsutsumi T．Yabuuchi 杜凯张厚琼张林唐永健中科院物理所光物理实验室中科院物理所光物理实验室中科院物理所光物理实验室中科院物理所光物理实验室中科院物理所光物理实验室 Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University Institute of laser Engineering Osaka University 中物院激光聚变研究中心中物院激光聚变研究中心中物院激光聚变研究中心中物院激光聚变研究中心

＜正＞引言当前超强激光产生的超热电子束远大于Alfven限,所以要想得到稳定的超热电子束的输运,背景冷电子回流必须能够满足电中性要求。固体靶中冷电子密度高,基本可以补偿目前所能产生的超热电子束传输。但是:实用级别的、满足快点火...

＜正＞引言当前超强激光产生的超热电子束远大于Alfven限,所以要想得到稳定的超热电子束的输运,背景冷电子回流必须能够满足电中性要求。固体靶中冷电子密度高,基本可以补偿目前所能产生的超热电子束传输。但是:实用级别的、满足快点火条件的超热电子束,其电子束密度和背景等离子体密度相当,此时冷电子回流不能平衡高密度超热电子流。泡沫靶背景电子密度低,可以补偿超热电子电中性的冷电子回流比固体靶中小,所以在目前的激光条件下,通过采用泡沫靶,可以模拟真实点火条件下的超热电子输运过程,加深对快点火概念的认识,了解低密度泡沫靶和固体靶相互作用的不同特点。

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Chinese Physics C 2020年第2期44卷 1-12页

作者： F.Abudinén I.Adachi P.Ahlburg H.Aihara N.Akopov A.Aloisio F.Ameli l.Andricek N.Anh Ky D.M.Asner H.Atmacan T.Aushev V.Aushev T.Aziz K.Azmi V.Babu S.Baehr S.Bahinipati A.M.Bakich P.Bambade Sw.Banerjee S.Bansal V.Bansal M.Barrett J.Baudot A.Beaulieu J.Becker P.K.Behera J.V.Bennett E.Bernieri F.U.Bernlochner M.Bertemes M.Bessner S.Bettarini V.Bhardwaj F.Bianchi T.Bilka S.Bilokin D.Biswas G.Bonvicini A.Bozek M.Bračko P.Branchini N.Braun T.E.Browder A.Budano S.Bussino M.Campajola l.Cao G.Casarosa C.Cecchi D.Červenkov M.-C.Chang P.Chang R.Cheaib V.Chekelian Y.Q.Chen Y.-T.Chen B.G.Cheon K.Chilikin H.-E.Cho K.Cho S.Cho S.-K.Choi S.Choudhury D.Cinabro l.Corona l.M.Cremaldi S.Cunliffe T.Czank F.Dattola E.De la Cruz-Burelo G.De Nardo M.De Nuccio G.De Pietro R.de Sangro M.Destefanis S.Dey A.De Yta-Hernandez F.Di Capua S.Di Carlo J.Dingfelder Z.Doležal I.Domínguez Jiménez T.V.Dong K.Dort S.Dubey S.Duell S.Eidelman M.Eliachevitch T.Ferber D.Ferlewicz G.Finocchiaro S.Fiore A.Fodor F.Forti A.Frey B.G.Fulsom M.Gabriel E.Ganiev M.Garcia-Hernandez R.Garg A.Garmash V.Gaur A.Gaz U.Gebauer A.Gellrich J.Gemmler T.Geßler R.Giordano A.Giri B.Gobbo R.Godang P.Goldenzweig B.Golob P.Gomis P.Grace W.Gradl E.Graziani D.Greenwald C.Hadjivasiliou S.Halder K.Hara T.Hara O.Hartbrich K.Hayasaka H.Hayashii C.Hearty M.T.Hedges I.Heredia de la Cruz M.Hernández Villanueva A.Hershenhorn T.Higuchi E.C.Hill H.Hirata M.Hoek S.Hollitt T.Hotta C.-l.Hsu Y.Hu K.Huang T.Iijima K.Inami G.Inguglia J.Irakkathil Jabbar A.Ishikawa R.Itoh M.Iwasaki Y.Iwasaki S.Iwata P.Jackson W.W.Jacobs D.E.Jaffe E.-J.Jang H.B.Jeon S.Jia Y.Jin C.Joo J.Kahn H.Kakuno A.B.Kaliyar G.Karyan Y.Kato T.Kawasaki H.Kichimi C.Kiesling B.H.Kim C.-H.Kim D.Y.Kim S.-H.Kim Y.K.Kim Y.Kim T.D.Kimmel K.Kinoshita C.Kleinwort B.Knysh P.Kodyš T.Koga I.Komarov T.Konno S.Korpar D.Kotchetkov N.Kovalchuk T.M.G.Kraetzschmar P.Križan R.Kroeger J.F.Krohn P.Krokovny W.Kuehn T.Kuhr M.Kumar R.Kumar K.Kumara S.Kurz A.Kuzmin Y.-J.Kwon S.lacaprara Y.-T.lai C.la licata K.lalwani l.lanceri J.S.lange K.lautenbach I.-S.le Beihang University Beijing 100191 Brookhaven National laboratory UptonNew York 11973 Budker Institute of Nuclear Physics SB RAS Novosibirsk 630090 Centro de Investigacion y de Estudios Avanzados del Instituto Politecnico Nacional Mexico City 07360 Faculty of Mathematics and Physics Charles University12116 Prague Chiba University Chiba 263-8522 Consejo Nacional de Ciencia y Tecnología Mexico City 03940 Deutsches Elektronen–Synchrotron 22607 Hamburg Duke University DurhamNorth Carolina 27708 Earthquake Research Institute University of TokyoTokyo 113-0032 Forschungszentrum Jülich 52425 Jülich Department of Physics Fu Jen Catholic UniversityTaipei 24205 Key laboratory of Nuclear Physics and Ion-beam Application(MOE)and Institute of Modern Physics Fudan UniversityShanghai 200443 II.Physikalisches Institut Georg-August-Universität Göttingen37073 Göttingen Gifu University Gifu 501-1193 The Graduate University for Advanced Studies(SOKENDAI) Hayama 240-0193 Gyeongsang National University Jinju 52828 Department of Physics and Institute of Natural Sciences Hanyang UniversitySeoul 04763 High Energy Accelerator Research Organization(KEK) Tsukuba 305-0801 J-PARC Branch KEK Theory CenterHigh Energy Accelerator Research Organization(KEK)Tsukuba 305-0801 Indian Institute of Science Education and Research Mohali SAS Nagar140306 Indian Institute of Technology Bhubaneswar Satya Nagar 751007 Indian Institute of Technology Hyderabad Telangana 502285 Indian Institute of Technology Madras Chennai 600036 Indiana University BloomingtonIndiana 47408 Institute for High Energy Physics Protvino 142281 Institute of High Energy Physics Vienna 1050 Institute of High Energy Physics Chinese Academy of SciencesBeijing 100049 Institute of Particle Physics(Canada) VictoriaBritish Columbia V8W 2Y2 Institute of Physics Hanoi Instituto de Fisica Corpuscular Paterna 46980 INFN laboratori Nazionali di Frascati I-00044 Frascati INFN Sezione di Napoli I-80126 Napoli INFN Sezione di Padova I-35131 Padova INFN Sezione di Perugia I-06123 Perugia

From April to July 2018,a data sample at the peak energy of the T(4 S) resonance was collected with the Belle Ⅱ detector at the SuperKEKB electron-positron *** is the first data sample of the Belle Ⅱ *** Bhabha and digamma events,we measure the integrated luminosity of the data sample to be(496.3±0.3±3.0) pb-1,where the first uncertainty is statistical and the second is *** work provides a basis for future luminosity measurements at Belle Ⅱ.

关键词： luminosity Bhabha digamma Belle II