|
|
|
题名
|
作者
|
年代
|
出处
|
被引量
|
| 1 | 北京清华园采暖前与采暖期PM_(10)中含碳组分的理化特征显示文摘采用美国rp公司生产的Series5400大气颗粒物碳质组分监测仪对清华园PM10中的碳质组分进行了连续在线监测(2002年9月-11月)。结合PM2.5中碳质组分浓度、PM10的浓度和气象数据,分析了碳质组分的污染特征。结果表明,采样期间清华园大气PM10中有机碳(OC)、元素碳(EC)的日平均质量浓度分别在4.07~65.81μg/m^3、0.96~26.14μg/m^3之间变化,平均值分别为20.8±12.1和7.0±5.1μg/m^3。OC在总碳(TC)中占有很大比例,OC/TC平均值为75.84%;TC在PM10中的含量平均为25.0%。本文对9—10月份(秋季)和11月份(初冬)OC、EC的相关性分别进行了分析,结果表明OC、EC之间具有良好的相关性,9月份和10月份相关性系数(R^2)为0.83;11月份为0.90。二次生成的OC(OCsec)浓度估算结果表明,9、10月份OCsec在OC中的比例(60.7%)比11月份(38.5%)大。碳质组分主要集中在细颗粒物中,PM10中的OC有70.3%存在于细颗粒物PM2.5中,TC则有58.6%存在于PM2.5中。 | 贾英韬 贺克斌 马永亮 杨复沫 段凤魁 雷宇 S.Tanaka T.Okuda | 2006 | 中国环境监测2006，22，4： | 9 |
| 2 | Measurement of the integrated luminosity of the Phase 2 data of the Belle Ⅱ experiment显示文摘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 collider.This is the first data sample of the Belle Ⅱ experiment.Using 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 systematic.This work provides a basis for future luminosity measurements at Belle Ⅱ. | 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.Lee S.C.Lee P.Leitl D.Levit P.M.Lewis C.Li L.K.Li S.X.Li Y.M.Li Y.B.Li J.Libby K.Lieret L.Li Gioi J.Lin Z.Liptak Q.Y.Liu D.Liventsev S.Longo A.Loos F.Luetticke T.Luo C.MacQueen Y.Maeda M.Maggiora S.Maity E.Manoni S.Marcello C.Marinas A.Martini M.Masuda K.Matsuoka D.Matvienko J.McNeil J.C.Mei F.Meier M.Merola F.Metzner M.Milesi C.Miller K.Miyabayashi H.Miyata R.Mizuk G.B.Mohanty H.Moon T.Morii H.-G.Moser F.Mueller F.J.Müller Th.Muller R.Mussa K.R.Nakamura E.Nakano M.Nakao H.Nakayama H.Nakazawa M.Nayak G.Nazaryan D.Neverov M.Niiyama N.K.Nisar S.Nishida K.Nishimura M.Nishimura M.H.A.Nouxman B.Oberhof S.Ogawa Y.Onishchuk H.Ono Y.Onuki P.Oskin H.Ozaki P.Pakhlov G.Pakhlova A.Paladino T.Pang E.Paoloni H.Park S.-H.Park B.Paschen A.Passeri S.Patra S.Paul T.K.Pedlar I.Peruzzi R.Peschke R.Pestotnik M.Piccolo L.E.Piilonen P.L.M.Podesta-Lerma V.Popov C.Praz E.Prencipe M.T.Prim M.V.Purohit P.Rados M.Remnev P.K.Resmi I.Ripp-Baudot M.Ritter M.Ritzert G.Rizzo L.B.Rizzuto S.H.Robertson D.Rodríguez Pérez J.M.Roney C.Rosenfeld A.Rostomyan N.Rout G.Russo D.Sahoo Y.Sakai D.A.Sanders S.Sandilya A.Sangal L.Santelj P.Sartori Y.Sato V.Savinov B.Scavino M.Schram H.Schreeck J.Schueler C.Schwanda A.J.Schwartz B.Schwenker R.M.Seddon Y.Seino A.Selce K.Senyo M.E.Sevior C.Sfienti C.P.Shen H.Shibuya J.-G.Shiu A.Sibidanov F.Simon S.Skambraks R.J.Sobie A.Soffer A.Sokolov E.Solovieva S.Spataro B.Spruck M.Starič S.Stefkova Z.S.Stottler R.Stroili J.Strube M.Sumihama T.Sumiyoshi D.J.Summers W.Sutcliffe M.Tabata M.Takizawa U.Tamponi S.Tanaka K.Tanida H.Tanigawa N.Taniguchi Y.Tao P.Taras F.Tenchini E.Torassa K.Trabelsi T.Tsuboyama N.Tsuzuki M.Uchida I.Ueda S.Uehara T.Uglov K.Unger Y.Unno S.Uno P.Urquijo Y.Ushiroda S.E.Vahsen R.van Tonder G.S.Varner K.E.Varvell A.Vinokurova L.Vitale A.Vossen E.Waheed H.M.Wakeling K.Wan W.Wan Abdullah B.Wang M.-Z.Wang X.L.Wang A.Warburton M.Watanabe S.Watanuki J.Webb S.Wehle N.Wermes C.Wessel J.Wiechczynski P.Wieduwilt H.Windel E.Won S.Yamada W.Yan S.B.Yang H.Ye J.Yelton J.H.Yin M.Yonenaga Y.M.Yook C.Z.Yuan Y.Yusa L.Zani J.Z.Zhang Z.Zhang V.Zhilich Q.D.Zhou X.Y.Zhou V.I.Zhukova V.Zhulanov A.Zupanc | 2020 | Chinese Physics C2020，44，2： | 2 |
| 3 | 地球潮汐能够触发浅源逆冲断层地震显示文摘说明了浅源逆冲断层地震的发生与最强烈潮汐的出现存在相关性。在潮汐应力作用下,地震速率以因子3随背景速率而变化。尽管摩擦系数μ在0.2和0.6之间时我们看到了好的相关性,但最高的相关性是在假定地壳的μ=0.4时发现的。我们的结果量化了所施加应力在地震触发上的效应,在理解地震成核与重复发生上,这是一个关键因素,地震由此被触发并接二连三地发生。 | E.S.Cochran J.E.Vidale S.Tanaka 朱大庆(译) 邹本良(译) 李世愚(校) | 2006 | 世界地震译丛2006，37，2： | 1 |
| 4 | 日本软岩边坡工程的新发展显示文摘日本是一个多滑坡灾难的国家,也是一个有着丰富研究滑坡经验的国家,多年来对各种起因的滑坡破坏现象进行了大量的调查,在研究技术上也取得了很大进展,并能在设计领域里科学地加以控制。 | K.Kikuchi Y.Kitahara H.Nakamura S.Tanaka O.Tsuruta R.Yoshinaka 魏嘉昆 | 1989 | 露天采矿技术1989，，2： | 0 |
| 5 | 日本软岩边坡工程的新发展(续)显示文摘2.力学性质图4表明设计方法的应用与力学性质密切结合,特别是:滑弧和复杂滑动面方法,剪切强度;有限元的静态分析,强度和形变特征,包括应力、应变间的关系。有限元法的动态分析,动态剪切强度,动态形变率和衰减系数,必要时,对动态应变强度提出再定量。这些力学性质能够由现场试验获得的结果来较好地确定。(1)关于强度或变形特性,许多作者已经提出过理论的或实际的经验公式。 | K.Kikuchi Y.Kitahara H.Nakamura S.Tanaka O.Tsuruta R.Yoshinaka 魏嘉昆 | 1989 | 露天采矿技术1989，，3： | 0 |
| 6 | 中型车用发动机DPR-Ⅱ排气后处理系统显示文摘日本开发了一种不采用尿素溶液的名为“DPR-Ⅱ”的排气后处理系统。该系统采用柴油作为碳氢-选择性催化还原(HC-SCR)的还原剂来减少柴油机排气中的氮氧化物(NOx)。这项基本技术能在宽广的温度范围内产生很好的NOx还原性能,以达到日本2016年排放法规要求。 | 朱炳全(译) | 2019 | 汽车与新动力2019，2，4： | 0 |
| 7 | Grain size refinement of magnesium composite alloys by addition of B_2O_3显示文摘The high performance magnesium alloy was investigated by adding B2O3 in magnesium and magnesium alloys. Experiments include adding B2O3 in Mg, Mg-Al and Mg-RE alloys, respectively, studying the effects of B2O3 on the microstructure, were studied measuring the change of grain size and microhardness of the materials, discussing the change of grain size, morphology and distribution. The results show that adding 3% or 6%(mass fraction) B2O3 in Mg can bring twinning in Mg, adding B2O3 in Mg-Al alloys and Mg-RE alloys can refine the alloy grain size. Adding 3%B2O3 in Mg-6Al alloys can refine the average grain size by about 5μm, with the average hardness increased by 13.3% (53.3-60.4 HV0.03); adding 6%B2O3 in Mg-6Al alloys can refine the average grain size by about 13μm, with the average hardness increased by 15.8% (53.3-61.73 HV0.03); adding 3% and 6%B2O3 into Mg-6RE alloys can refine the grain size by about 5 and 9μm, respectively, with the average hardness decreased to HV0.03 64.66 and HV0.03 57.86, respectively from HV0.03 88.57. In the Mg-6Al alloy the content of aluminum is increased, while in the Mg-6RE alloy the content of oxygen is decreased. It can be concluded that it is beneficial to develop Mg-Al-B-O particle reinforce composite alloys, and it is feasible to develop nanometer crystallization of block material by Mg-B-O-RE. | 卜乐平 S.TANAKA M.TSUSHIDA S.ANDO H.TONDA | 2006 | 中国有色金属学会会刊:英文版2006，16，A03： | 0 |
| 8 | Development of magnesium composite alloy by a new method combining B_2O_3 addition and melt stirring显示文摘For developing high performance magnesium alloys, a new method in combination of B2O3 addition and melt stirring was applied. When 0, 3%, 6% and 12%( mass fraction) B2O3 was added into pure Mg, many twins were produced in each alloy. The average grain size of Mg was about 200μm. In Mg-6Al alloy, the grain size is decreased from 50 to 35μm by B2O3 addition. In Mg-6RE (rare earth) alloys, the grain size is decreased from 35 to 15μm. The grain size of Mg-9Al- 6Ti-3B2O3 alloy is about 5μm. The hardness of pure Mg does not change by B2O3 addition. In Mg-6Al alloy, the hardness is increased by addition of 3% B2O3, however, the hardness of Mg-6RE alloy is decreased by B2O3 addition. Addition of B2O3 into Mg-Al, Mg-RE and Mg-Al-Ti alloys makes the fine grain structures, the hardness of Mg-RE alloy is decreased. This strange behavior may be interpreted with existence of many fine pores in the alloy. The mechanical properties of composite Mg-9Al-6Ti with 3%B2O3 are higher than those of AZ91C. The present results demonstrate the potential of this new method for developing high performance magnesium alloys. | 卜乐平 S.TANAKA M.TSUSHIDA S.ANDO H.TONDA | 2006 | 中国有色金属学会会刊:英文版2006，16，A03： | 0 |
您所在的机构暂未开通此部分的功能，请联系管理员