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Inorganic Elements in Eggs of Two Cavity-Nesting Passerine Species at and around Los Alamos National Laboratory, Los Alamos, New Mexico

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Journal of Environmental Protection 2018年第9期9卷 932-947页

作者： Shannon Marie Gaukler charles dean Hathcock Jeanne Marie Fair Environmental Stewardship Group Los Alamos National Laboratory Los Alamos NM USA Biosecurity and Public Health Los Alamos National Laboratory Los Alamos NM USA

Los Alamos National Laboratory (LANL) was established in 1943 as part of the Manhattan Project to build nuclear weapons, and currently operates as a national research laboratory. As part of an ongoing assessment of site-related ecological risk at LANL, western bluebird (Sialia mexicana) and ash-throated flycatcher (Myiarchus cinerascens) eggs were collected from 1997 to 2012 and analyzed for 18 inorganic elements. Concentrations of many inorganic elements in eggs were below reporting limits. Between species comparisons revealed that western bluebird eggs had higher levels of barium while ash-throated flycatcher eggs had higher levels of mercury. No statistically significant differences were observed in concentrations of inorganic elements in western bluebird eggs collected from the study area (which consists of areas within the current and historic LANL boundary) and from a non-industrial reference site;nor were any statistically significant differences observed between two canyons of interest, known to have received effluents and storm water runoff from LANL facilities, and the non-industrial reference site. Inorganic element levels detected in western bluebirds were typically within the range measured in eggs of other passerine in the published literature. These data suggest that concentrations of inorganic elements in passerine eggs collected from the study area appear to be at levels causing negligible risks to local bird populations.

关键词： Ash-Throated Flycatcher Biomonitoring Metals Western Bluebird

Medium-chain fatty acids and monoglycerides as feed additives for pig production:towards gut health improvement and feed pathogen mitigation

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Journal of Animal Science and Biotechnology 2020年第3期11卷 611-625页

作者： Joshua A.Jackman Rdean Boyd charles C.Elrod School of Chemical Engineering Sungkyunkwan UniversitySuwon 16419Republic of Korea Hanor Company FranklinKY 42134USA North Carolina State University RaleighNC 27695USA Natural Biologics Inc. NewfieldNY 14867USA Department of Animal Science Cornell UniversityIthacaNY 14853USA.

Ongoing challenges in the swine industry,such as reduced access to antibiotics and virus outbreaks(e.g.,porcine epidemic diarrhea virus,African swine fever virus),have prompted calls for innovative feed additives to support pig ***-chain fatty acids(MCFAs)and monoglycerides have emerged as a potential option due to key molecular features and versatile functions,including inhibitory activity against viral and bacterial *** this review,we summarize recent studies examining the potential of MCFAs and monoglycerides as feed additives to improve pig gut health and to mitigate feed *** molecular properties and biological functions of MCFAs and monoglycerides are first introduced along with an overview of intervention needs at different stages of pig *** latest progress in testing MCFAs and monoglycerides as feed additives in pig diets is then presented,and their effects on a wide range of production issues,such as growth performance,pathogenic infections,and gut health,are *** utilization of MCFAs and monoglycerides together with other feed additives such as organic acids and probiotics is also described,along with advances in molecular encapsulation and delivery ***,we discuss how MCFAs and monoglycerides demonstrate potential for feed pathogen mitigation to curb disease *** forward,we envision that MCFAs and monoglycerides may become an important class of feed additives in pig production for gut health improvement and feed pathogen mitigation.

关键词： Antibiotics Feed pathogen mitigation Growth promotion Gut health Immune enhancement MCFA Medium-chain fatty acids Monoglycerides

Shock standards Cu, Ag, Ir, and Pt in a wide pressure range

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Matter and Radiation at Extremes 2023年第4期8卷 37-46页

作者： Leonid Burakovsky dean L.Preston Scott D.Ramsey charles E.Starrett Roy S.Baty Los Alamos National Laboratory Los AlamosNew Mexico 87545USA

Although they are polymorphic(multiphase)materials,both copper and silver are reliable Hugoniot standards,and thus it is necessary to establish an accurate analytic model of their principal *** we present analytic forms of their principal Hugoniots,as well as those of iridium and platinum,two“pusher”standards for shock-ramp experiments,over a wide range of *** are based on our new analytic model of the principal Hugoniot[Burakovsky et al.,***.132,215109(2022)].Comparison of the four Hugoniots with experimental and independent theoretical data(such data exist to very high pressures for both copper and silver)demonstrates excellent ***,the new model for copper and silver can be considered as providing the corresponding Hugoniot standards over a wide pressure *** also suggest an approach for calculating the Grüneisen parameter along the Hugoniot and apply it to copper as a prototype,and our results appear to be in good agreement with the available data.

关键词： silver copper analytic

Ultra-broadband and polarization-independent planar absorber based on multilayered graphene

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Chinese Physics B 2017年第11期26卷 186-192页

作者：王娇高超宁姜彦南 charles Nwakanma Akwuruoha Guangxi Key Laboratory of Wireless Wideband Communication and Signal Processing Key Laboratory of Cognitive Radio and Information Processing (Ministry of Education) Guilin University of Electronic Technology School of Electrical and Electronic Engineering University of Manchester

We propose an ultra-broadband and polarization independent planar absorber comprising multilayered graphene. The bandwidth of the proposed absorber is extended by increasing the number of layers of graphene, and it is polarization independent due to its symmetrical unit structure. The full wave simulation results show that an absorber with three graphenebased layers can efficiently harvest an electromagnetic wave with random polarization from 17.9 GHz to 188.7 GHz（i.e.,covering frequency regimes from K to D bands and relative bandwidth of - 165%）. The physical absorption mechanism of ultra-broadband absorption has been elaborated upon using the destructive interference method and multiple resonances approach in a multilayered medium. The proposed absorber can be used in many applications such as medical treatment,electromagnetic compatibility, and stealth technique.

关键词： multilayered graphene absorber ultra-broadband polarization independent

Parallelization of Diagnostics for Climate Model Development

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Journal of Software Engineering and Applications 2016年第5期9卷 199-207页

作者： Jim McEnerney Sasha Ames Cameron Christensen charles Doutriaux Tony Hoang Jeff Painter Brian Smith Zeshawn Shaheen dean Williams Lawrence Livermore National Laboratory Livermore California USA University of Utah Salt Lake City Utah USA Oak Ridge National Laboratory Oak Ridge Tennessee USA

The parallelization of the diagnostics for climate research has been an important goal in the performance testing and improvement of the diagnostics for the Department of Energy’s (DOE’s) Accelerated Climate Modeling for Energy (ACME) project [1]. The primary mission of the ACME project is to build and test the next-generation Earth system model for current and future generations of computing systems operated by the DOE office of science computing facilities, including the envisioned exascale systems foreseen in the early part of the next decade. As part of the underpinning workflow environment, a diagnostics, model metrics, and intercomparison Python framework, called UVC Metrics was created to aid in testing and production execution of the model. This framework builds on common methods and similar metrics to accommodate and diagnose individual component models, such as atmosphere, land, ocean, sea ice, and land ice. This paper reports on initial parallelization of UVC Metrics for the atmosphere model component using two popular frameworks: MPI and SPARK. A timing study is presented to assess the performance of each method in which significant improvement was achieved for both frameworks despite I/O contentions with NFS. The advantages and disadvantages of each framework are also presented.

关键词： Climate Diagnostics Parallel MPI SPARK

遗产旅游的经济价值:澳大利亚阿利斯·斯普林斯(Alice Springs)的案例(英文)

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旅游学研究

旅游学研究 2007年 41-48页

作者： dean Carson Fiona Richards Susan Lee Morag McGrath charles Darwin University Tourism Research Group charles Darwin University International Marketing Office Tourism Northern Territory charles Darwin University School of Tourism and Hospitality

阿利斯·斯普林斯位于澳大利亚中部,它凭借邻近Uluru(乌卢鲁)、Kata Tjuta(奥尔加)和Wa-tarrka(国王大峡谷)等重要的自然吸引物的地理优势而成为一个发展良好的旅游目的地。最近到阿利斯·斯普林斯的旅游者的停留时间有明显下降的趋势... 详细信息

阿利斯·斯普林斯位于澳大利亚中部,它凭借邻近Uluru(乌卢鲁)、Kata Tjuta(奥尔加)和Wa-tarrka(国王大峡谷)等重要的自然吸引物的地理优势而成为一个发展良好的旅游目的地。最近到阿利斯·斯普林斯的旅游者的停留时间有明显下降的趋势。当地的遗产资源的利用已经被目的地的营销组织北部旅游(Tourism Northern Territory)所确定,并将此作为鼓励旅游者停留更长时间的方式。在准备遗产旅游行动计划的过程中,北部旅游(Tourism Northern Territory)委托查理斯·达尔文大学对这一地区的遗产旅游的现有经济价值和遗产旅游进一步发展的潜力进行了评估。本研究采用了先前用来评价国家公园的旅游价值的经济建模方法揭示了在阿利斯·斯普林斯的10 %以上的旅游支出可以归因于遗产旅游。这一研究表明,单纯的产品展示活动和对于维护遗产旅游资源的无偿部分的依赖等因素所占比重相对较低。产品开发、包装和销售等方面的创新对于阿利斯·斯普林斯提高遗产旅游的价值是很有必要的。

关键词：遗产旅游澳大利亚经济冲击创新

初生期异氟烷暴露对小鼠脑细胞发育、成年期行为、学习和记忆的影响

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麻醉与镇痛 2011年第2期7卷 55-69,77页

作者： Andreas W. Loepke, MD, PhD, FAAP George K. Istaphanous, MD John J. McAuliffe, Ⅲ, MD, MBA, FAAP Lili Miles, MD Elizabeth A. Hughes, BS lohn C. McCann, BS Kathrvn E. Harlow, BS C. dean Kurth, MD, FAAP Michael T. Williams, PhD charles V. Vorhees, PhD Steve C. Danzer, PhD 黎平(译) 闵苏(校) Departments of Anesthesia University of Cincinnati College of Medidne Cindnnati Ohio Pathology Cincinnati Children's Hospital Medical Center and University of Cincinnati College of Medidne Cindnnati Ohio Department of Anesthesia Cincinnati Children's Hospital Medical Center Cindnnati Ohio Department of Pediatrics Division of Neurology Cindnnati Children's Research Foundation and University of Cindnnati College of Medidne Cindnnati Ohio 不详

背景异氟烷等吸入麻醉药广泛地应用于婴幼儿。异氟烷、咪达唑仑以及氧化亚氮暴露后，新生小鼠神经变性和神经认知功能损害的一些研究，已经引起越来越多人对儿科麻醉安全问题的关注。新生小鼠异氟烷暴露较长时间会触发可致神经认知功能... 详细信息

背景异氟烷等吸入麻醉药广泛地应用于婴幼儿。异氟烷、咪达唑仑以及氧化亚氮暴露后，新生小鼠神经变性和神经认知功能损害的一些研究，已经引起越来越多人对儿科麻醉安全问题的关注。新生小鼠异氟烷暴露较长时间会触发可致神经认知功能损害的低血糖症。本研究即检测初生期异氟烷暴露和血糖对小鼠的脑细胞存活力、自主活动能力以及空间学习记忆能力的影响。方法出生7天的小鼠随机分配到1．5％异氟烷暴露6小时麻醉组、麻醉并注射葡萄糖组、麻醉并注射生理盐水组和空气暴露不麻醉组。检测动脉血气和血糖。暴露处理后2小时及18小时、11周，脑片染色检测Fluoro-JadeB、caspase3以及NeuN，评价脑细胞存活力。吸入麻醉剂暴露9周后，评价自主活动能力，Morris水迷宫法隐藏平台试验和颠倒平台试验评价空间学习记忆能力。结果与不麻醉组相比，其余组动物几个脑区的细胞凋亡在异氟烷暴露后早期增加。在两个受初生期变性影响显著的脑区，尽管发现新生小鼠暴露后细胞消失，但神经元密度在成年后没有明显差异。各组小鼠成年期的自主活动能力、空间学习记忆能力相似，与初生期异氟烷暴露无关。初生期异氟烷暴露导致18％的死亡率、短暂的PaCO2及乳酸升高、碱缺失以及血糖水平降低。但低血糖似乎不会引起神经退行性变，因为补充葡萄糖未能阻止神经元丢失。结论小鼠较长时间的初生期异氟烷暴露引起早期神经细胞变性增加，但成年期神经元密度并无显著减少，自主活动能力和空间学习记忆能力无明显损害。

关键词：空间学习记忆能力异氟烷细胞发育成年期初生鼠脑 Morris水迷宫法认知功能损害

Search for the rare decay B^(0)→J/ψФ

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Chinese Physics C 2021年第4期45卷 47-60页

作者： R.Aaij C.Abellin Beteta T.Ackernley B.Adeva M.Adinolfi H.Afsharnial C.A.Aidala S.Aiola Z.Ajaltouni S.Akar J.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche G.Alkhazov P.Alvarez Cartelle S.Amato Y.Amhis L.An L.Anderlini A.Andreianov M.Andreotti F.Archilli A.Artamonov M.Artuso K.Arzymatov E.Aslanides M.Atzeni B.Audurier S.Bachmann M.Bachmaver J.J.Back S.Baker P.Baladron Rodriguez V.Balagura W.Baldinit J.Baptista Leite R.J.Barlow S.Barsuk W.Barter M.Bartolini F.Baryshnikov J.M.Basels G.Bassi B.Batsukh A.Battig A.Bay M.Becker F.Bedeschis I.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Bencivenni E.Ben-Haim A.Berezhnoy *** D.Berninghoff H.C.Bernstein C.Bertella E.Bertholet A.Bertolin C.Betancourt F.Betti M.O.Bettler Ia.Bezshyiko S.Bhasin J.Bhom L.Bian M.S.Bieker S.Bifani P.Billoir M.Birch F.C.R.Bishop A.Bizzeti M.Biorn M.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska J.A.Boelhauve O.Boente Garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar S.Borghi M.Borisyak M.Borsato J.T.Borsuk S.A.Bouchiba T.J.V.Bowcock A.Boyer C.Bozzi M.J.Bradley S.Braun A.Brea Rodriguezs M.Brodski J.Brodzicka A.Brossa Gonzalo D.Brundu A.Buonaura C.Burr A.Burschee A.Butkevich J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calefice L.Calero Diaz S.Cali R.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes A.Camboni P.Campana D.H.Campora Perez A.F.Campoverde Quezada S.Capelli L.Capriotti A.Carbonel G.Carboni R.Cardinale A.Cardini I.Carli P.Carniti L.Carus K.Carvalho Akiba A.Casais Vidal G.Casse M.Cattaneo G.Cavallero S.Celani J.Cerasoli A.J.Chadwick M.G.Chapman M.charles Ph.Charpentier G.Chatzikonstantinidis C.A.Chavez Barajas M.Chefdeville C.Chen S.Chen A.Chernov S.-G.Chitic V.Chobanova S.Cholak M.Chrzaszcz A.Chubykin V.Chulikov P.Ciambrone M.F.Cicala X.Cid Vidal G.Ciezarek P.E.L.Clarke M.Clemencic H.V.Cliff J.Closier J.L.Cobbledick V.Coco J.A.B.Coelho J.Cogan E.Cogneras L.Cojocariu P.Collins T.Colombo L.Congedo A.Contu N.Cooke G.Coombs G.Corti C.M.Costa Sobral B.Couturier D.C.Craik J.Crkovska M.Cruz Centro Brasileiro de Pesquisas Fisicas(CBPF) Riode JaneiroBrazil Universidade Federal do Riode Janeiro(UFRJ) Riode JaneiroBrazil Center for High Energy Physics Tsinghua UniversityBeijingChina School of Physics State Key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University of Chinese Academy of Sciences BeijingChina Institute Of High Energy Physics(IHEP) BejingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.Grenoble Alpes Univ.Savoie Mont BlancCNRSIN2P3-LAPPAnnecyFrance Universite Clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix Marseille Univ CNRS/IN2P3CPPMMarseilleFrance Universitq Paris-Saclay CNRS/IN2P3IJCLabOrsayFrance LPNHE Sorbonne UniversiteParis Diderot Sorbonne Paris CiteCNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany Max-Planck-Institut fir Kernphysik(MPIK) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universitat HeidelbergHeidelbergGermany School of Physics University College DublinDublinIreland INFN Sezione di Bari BariItaly INFN Sezione di Bologna BolognaItaly INFN Sezione di Ferrara FerraraItaly INFN Sezione di Firenze FirenzeItaly INFN Laboratori Nazionali di Frascati Frascatiltaly INFN Sezione di Genova GenovaItaly INFN Sezione di Milano Bicocca Milanolaly INFN Sezione di Milano MilanoItaly INFN Sezione di Cagliari Monserratoltaly Universita degli Studi di Padova Universita e INFNPadovaPadovaItaly INFN Sezione di Pisa PisaItaly INFN Sezione di Roma Tor Vergata RomaItaly INFN Sezione di Roma La Sapienza RomaItaly Nikhef National Institute for Subatomic Physics AmsterdamNetherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam AmsterdamNetherlands Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences KrakowPoland AGH-University of Science and Technology Faculty of Physics and Applied Computer Science

A search for the rare decay B^(0)→J/ψФis performed using Pp collision data collected with the LHCb dete-ctor at centre-of-mass energies of 7,8 and 13 TeV,corresponding to an integrated luminosity of9 *** significant signal of the decay is observed and an upper limitof 1.1x 10^(-7)at 90%confidence level is set on the branching fraction.

关键词： B physics flavour physics rare decay ω-Фmixing branching fraction

Search for the doubly heavy baryons Ωbc0 and Ξbc0 decaying to Λc+π- and Ξc+π-

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Chinese Physics C 2021年第9期45卷 14-25页

作者： R.Aaij C.Abellán Beteta T.Ackernley B.Adeva M.Adinolfi H.Afsharnia C.A.Aidala S.Aiola Z.Ajaltouni S.Akar J.Albrecht F.Alessio M.Alexander A.Alfonso Albero Z.Aliouche G.Alkhazov P.Alvarez Cartelle S.Amato Y.Amhis L.An L.Anderlini A.Andreianov M.Andreotti F.Archilli A.Artamonov M.Artuso K.Arzymatov E.Aslanides M.Atzeni B.Audurier S.Bachmann M.Bachmayer J.J.Back P.Baladron Rodriguez V.Balagura W.Baldini J.Baptista Leite R.J.Barlow S.Barsuk W.Barter M.Bartolini F.Baryshnikov J.M.Basels G.Bassi B.Batsukh A.Battig A.Bay M.Becker F.Bedeschi I.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Bencivenni E.Ben-Haim A.Berezhnoy *** D.Berninghoff H.C.Bernstein C.Bertella A.Bertolin C.Betancourt F.Betti Ia.Bezshyiko S.Bhasin J.Bhom L.Bian M.S.Bieker S.Bifani P.Billoir M.Birch F.C.R.Bishop A.Bitadze A.Bizzeti M.Bj?rn M.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska J.A.Boelhauve O.Boente Garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar S.Borghi M.Borisyak M.Borsato J.T.Borsuk S.A.Bouchiba T.J.V.Bowcock A.Boyer C.Bozzi M.J.Bradley S.Braun A.Brea Rodriguez M.Brodski J.Brodzicka A.Brossa Gonzalo D.Brundu A.Buonaura C.Burr A.Bursche A.Butkevich J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calefice L.Calero Diaz S.Cali R.Calladine M.Calvi M.Calvo Gomez P.Camargo Magalhaes A.Camboni P.Campana A.F.Campoverde Quezada S.Capelli L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini I.Carli P.Carniti L.Carus K.Carvalho Akiba A.Casais Vidal G.Casse M.Cattaneo G.Cavallero S.Celani J.Cerasoli A.J.Chadwick M.G.Chapman M.charles Ph.Charpentier G.Chatzikonstantinidis C.A.Chavez Barajas M.Chefdeville C.Chen S.Chen A.Chernov V.Chobanova S.Cholak M.Chrzaszcz A.Chubykin V.Chulikov P.Ciambrone M.F.Cicala X.Cid Vidal G.Ciezarek P.E.L.Clarke M.Clemencic H.V.Cliff J.Closier J.L.Cobbledick V.Coco J.A.B.Coelho J.Cogan E.Cogneras L.Cojocariu P.Collins T.Colombo L.Congedo A.Contu N.Cooke G.Coombs G.Corti C.M.Costa Sobral B.Couturier D.C.Craik J.Crkovská M.Cruz Torres R.Currie C.L.Da Silva E.Dall'Occo J.Dalseno C.D'Amb University of Edinburgh Horia Hulubei National Institute of Physics and Nuclear Engineering INFN Sezione di Bari Università di Bari Los Alamos National Laboratory (LANL) Van Swinderen Institute University of Groningen Universiteit Maastricht AGH-University of Science and Technology Faculty of Physics and Applied Computer Science Université Clermont Auvergne Università di Cagliari Institute for Nuclear Research of the National Academy of Sciences (KINR) School of Physics University College Dublin NSC Kharkiv Institute of Physics and Technology (NSC KIPT) INFN Sezione di Perugia STFC Rutherford Appleton Laboratory School of Physics and Astronomy Monash University Novosibirsk State University CNRS/IN2P3 Department of Physics and Astronomy Uppsala University Università di Genova School of Physics State Key Laboratory of Nuclear Physics and Technology Peking University National Center for Nuclear Research (NCBJ) Università di Roma Tor Vergata Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio) Universidade Federal do Triangulo Mineiro (UFTM) Institute of Particle Physics LPC Central China Normal University Hangzhou Institute for Advanced Study UCAS Instituto de Fisica Corpuscular Centro Mixto Universidad de Valencia-CSIC Nikhef National Institute for Subatomic Physics and VU University Amsterdam National Research Tomsk Polytechnic University AGH-University of Science and Technology Faculty of Computer Science Electronics and Telecommunications University of Michigan Università di Siena Università di Padova Scuola Normale Superiore National Research Centre Kurchatov Institute Università degli Studi di Milano MSU-Iligan Institute of Technology (MSU-IIT) Università di Firenze INFN Sezione di Roma La Sapienza Institut für Physik Universit?t Rostock INFN Sezione di Milano Departamento de Fisica Universidad Nacional de Colombia Universit?t Bonn-Helmholtz-Institut für Strahlen und Kernphysik Hanoi University of Science Università di Pisa P.N. Lebedev Physical Institute Russian Academy of Science (LPI RAS) Università

The first search for the doubly heavy Ωbc0baryon and a search for the Ξbc0baryon are performed using pp collision data collected via the LHCb experiment from 2016 to 2018 at a centre-of-mass energy of 13 TeV,corresponding to an integrated luminosity of 5.2 *** baryons are reconstructed via their decays to ∧c+π-andΞc+π-.No significant excess is found for invariant masses between 6700 and 7300 MeV/c2,in a rapidity range from2.0 to 4.5 and a transverse momentum range from 2 to 20 MeV/*** limits are set on the ratio of the Ωbc0andΞbc0production cross-section times the branching fraction to ∧c+π-（Ξc+π-） relative to that of the ∧b0（Ξb0） baryon,for different lifetime hypotheses,at 95% confidence *** upper limits range from 0.5×10-4to 2.5×10-4for theΩbc0→∧c+π-(Ξbc0→∧c+π-) decay,and from 1.4×10-3to 6.9×10-3for the Ωbc0→Ξc+π-(Ξbc0→Ξc+π-) decay,depending on the considered mass and lifetime of the Ωbc0(Ξbc0) baryon.

关键词： B physics quarkonium spectroscopy heavy quark production