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Natural Science 2011年第4期3卷 295-300页

作者： m. V. Egorova S. A. Afanasiev D. S. Kondratyeva B. N. Kozlov S. V. popov 不详

It was shown that the energy metabolism of the heart mitochondria of experimental animals and patients is more resistant to damage at combined postinfarction cardiosclerosis and diabetes in comparison with the individual pathology. We found that the changes of free fatty acid content and conjugation of the processes of oxidation and phosphorylation in heart mitochondria are components of the metabolic stability of myocardium at the combined development of postinfarction cardiosclerosis and diabetes mellitus. Our data demonstrate a direct link between the violations of the processes of oxidative phosphorylation and accumulation of free fatty acids owing to change in activity of endogenous phospholipases, in particularly, mi- tochondrial phospholipase A2. Similar results were obtained for intraoperative biopsy specimens of patients’ hearts, and of adult Wistar rats’ hearts. We hypothesized that the preservation of energy metabolism is a manifestation of summing up of compensatory processes at de- velopment of nonspecific response of cells to damage at the early stages of pathological pro- cess.

关键词： Postinfarction Remodeling Diabetes Heart mitochondria Fatty Acids Phospholipase A2

磷掺杂剂和石墨烯包覆层对NiCo_(2)S_(4)电催化剂析氢活性和耐久性的协同影响

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Science China materials 2023年第10期66卷 3875-3886页

作者：陈杰毛梁徐家琛顾修全 Zakhar I.popov 赵宇龙凌意瀚隋艳伟应鹏展蔡晓燕张俊英 School of materials Science and Physics China University of Mining and TechnologyXuzhou 221116China Emanuel Institute of Biochemical Physics RAS 1193344 Kosigin st.MoscowRussian Federation School of Physics Beihang UniversityBeijing 100191China

探索具有优异导电性和稳定性的非贵金属电催化剂对氢经济至关重要.本研究将杂原子掺杂和石墨烯包覆相结合,以控制NiCo_(2)S_(4)(NCS)蛋黄壳微球的电子性能,并抵抗酸性介质中H_(2)O和O_(2)的腐蚀.密度泛函理论(DFT)模拟结合综合表征和实... 详细信息

探索具有优异导电性和稳定性的非贵金属电催化剂对氢经济至关重要.本研究将杂原子掺杂和石墨烯包覆相结合,以控制NiCo_(2)S_(4)(NCS)蛋黄壳微球的电子性能,并抵抗酸性介质中H_(2)O和O_(2)的腐蚀.密度泛函理论(DFT)模拟结合综合表征和实验首次揭示了在NCS中引入P杂原子不仅加速了电子从体相向表面的转移动力学,而且降低了掺杂P原子附近活性S位上的析氢反应势垒.利用DFT计算的穿透能垒预测了rGO覆盖层在P掺杂NCS(P-NCS)表面对质子的渗透性和对H_(2)O和O_(2)分子的抵抗性等重要功能,并用X射线光电子能谱对新催化剂和回收催化剂进行了验证.利用P掺杂剂和rGO覆盖层分别辅助电荷传递和质子传递,通过二者的协同作用获得了催化活性和耐久性之间的平衡.因此,优化后的P-NCS/rGO在70 mV的低过电位下实现了10 mA cm^(-2)的电流密度,并具有令人满意的80小时耐用性.本工作阐明了石墨烯覆盖硫化物催化剂可通过调控电子结构和质子/分子穿透提高电催化性能.

关键词： electrocatalysis elemental doping proton penetration hydrogen evolution corrosion resistance

multiscale thin current sheets in the Eartyh’s magnetotail: the role of O+ ions.

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Multiscale thin current sheets in the Eartyh’s magnetotail:...

Comparative Study of the Anatomical Structure of Some Vegetative Organs <i>Allium caspium</i>(pall.) m. Bieb. and <i>Allium tschimganicum</i>B. Fedtsch. Ex popov Growing in Natural Conditions of Uzbekistan

第十一届全国日地空间物理学术讨论会

作者： malova H.V. Zelenyi L.m. popov V.Yu. Delcourt D.C. Ganushkina N.Yu. Sharma A.S. NPI mSU IKI RAS IKI RAS mSU CETP CNRS FmI maryland University USA

＜正＞Thin current sheets （TCSs） are known as sites of energy storage and release in the Earth’s magnetosphere. Self-consistent analytical model of multicomponent TCS has developed, where the tension of magnetic field lines is balanced by ion inertia rather than plasma pressure. The influence of electron population, which is quite fast enough to obey Boltzmann distribution along field lines, is taken into account. Electrostatic effects might lead to specific peculiarities of local current density profiles inside TCS, for example, to their splitting. It is shown that the contribution of oxygen ions in the total current is not very large, but current sheet becomes ten times more thickened. The dependence of these effects from electron and oxygen temperatures and the curvature of magnetic field lines are analyzed. Possible importance of these effects for the substorm processes in the Earth’s magnetotail is discussed.

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American Journal of Plant Sciences 2020年第9期11卷 1398-1404页

作者： Akida T. Abdullaeva Nargiza K. Rakhimova Guljan m. Duschanova Eldor E. Temirov Laboratory Anatomy and Cytoembryology of the Tashkent Botanical Garden Named after Academician F.N. Rusanov Institute of Botany of the Academy of Sciences Tashkent Uzbekistan

The results of a comparative study of the structure of some vegetative organs of A. caspium and A. tschimganicum growing in natural conditions in Uzbekistan are presented for the first time. During the study of the desert representative A. caspium, the following diagnostic, structural features were revealed: ribbing of the peduncle and pedicel;thickening of the outer wall of the epidermis and wavy folding of the cuticle of the parenchymal-bundle type of structure;deep submergence of stomata: extensive core: thinness of the crustal parenchyma, the presence of lactic acid in it;the presence of a highly sclerified sclerinchymal ring between the crustal parenchyma and the central cylinder: the vastness of the core and the presence of hydrocytic cells in it, as well as the similarity of the structure of the stem and pedicel. In this species, a predominance of xeromorphic characters was noted, due to a tendency indicating xerophilizationmily:Verdana;"> and adaptation to desert conditio

关键词： Anatomy Stem Pedicel Allium caspium Allium tschimganicum Samarkand Region Tashkent Region Uzbekistan

Diversity of nivicolous myxomycetes of the Teberda State Biosphere Reserve (Northwestern Caucasus,Russia)

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Fungal Diversity 2013年第2期59卷 109-130页

作者： Y.K.Novozhilov m.Schnittler D.A.Erastova m.V.Okun O.N.Schepin E.Heinrich Komarov Botanical Institute of the Russian Academy of Sciences Prof.Popov St.2197376 St.PetersburgRussia Institute of Botany and Landscape Ecology Ernst Moritz Arndt University GreifswaldGrimmer Str.8817487 GreifswaldGermany CIBIV–Center for Integrative Bioinformatics in Vienna Max F.Perutz Laboratories(MFPL)University of ViennaMedical University of ViennaCampus Vienna Biocenter 5(VBC5)1030 ViennaAustria

Nivicolous myxomycete assemblages were surveyed on the northwest of the Greater Caucasian ridge in may-June 2010 and 2011 at a north facing transect between 1,700 and 2,920 m elevation of the summit malaya Khatipara situated within the Teberda State Biosphere *** characters of 396 collections representing 45 taxa(39 species,3 varieties,and 3 forms)of myxomycetes in 8 genera and 5 families were ***(13)taxa are classified as rare(a species representsmore of the 17 studied localities).To confirm the assignment of specimens to morphospecies,we obtained independently from determination 145 partial sequences of the 18S SSU rRNA gene from 35 taxa of Lamproderma,meriderma,Physarum and Diderma,which turned out to represent 58 *** of the taxa represented by more than one sequence had several genotypes,with an average of 1.7 genotypes per *** for three taxonomically difficult groups of species,partial SSU sequences did well correspond with the respective morphospecies and where similar or identical to sequences of specimens from the European Alps,making this marker a good candidate for barcoding in *** richness and diversity increased from subalpine crooked-stem birch forests(23 species,2 varieties,H′02.8,E00.88,D00.08)to alpine dwarf shrub communities(34 species and 2 varieties,2 forms,H′03.2,E00.89,D00.05)but decreased again for alpine meadows(27 species and 2 varieties,2 forms,H′03.1,E00.91,D00.06).Species richness and alpha-diversity reached maximum values for ground litter,whereas leaves and stems of living shrubs above ground harboured a more depauperate myxomycete assemblage.

关键词： Alpine ecosystems Distribution Genotypes molecular signatures myxogastria Amoebozoa Plasmodial slime moulds Species inventory Species richness Species delimitation

POSSIBILITIES TO mODIFY AV CONDUCTION IN ATRIAL FIBRILLATION PATIENTS

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中国介入心脏病学杂志 1998年第4期6卷 165-165页

作者： I.V.Antonchenko S.V.popov G.m.Savenkova V.V.Aleev Institute of Cardiology TomskRussia

most of atrial fibrillation(AF)pts have organic artrial injury which ismaintained at modified AV conduction as an AV *** this procedure allows to control ventricular contractionsrate(VCR)in AF *** that "slow" pathways potentials arepotentials of atrial fibers eonneated with the AV node we used highfrequency current in the meadseptal right atrial area in 24 pts aged 52-74(mean 66±4.9 yrs)having paroxysmal(n=16)and chronic(n=8)*** was induced in pts who had sinus rhythm before ablation andif VSR exceeded 50-70 beats/min the procedure was *** results were obtained in 18(75% of pts).These pts didnot reveal decreased Wenekebach point or increased effectiverefractory period of the AV *** decreased from 163±27 to65±9(p=0.001)during *** atropine was given and if VSRexceeded 120/min we considered the procedure to be *** and beta-blockers which were ineffective before ablationbecame effective to control VSR after *** 6 to 12 months afterthe procedure,these pts underwent exercise testing(AF was inducedin the sinus rhythm pts):maximum VCR was 116±10.8/*** the procedure inefficacy,complete AV block was reached duringablation in 2(8%)pts in whom artificial pacemaker was *** modification of AV conduction is an effective procedure tocontrol VSR in AF pts and allows to flee 75% of pts fromantiarrhythmic drugs.

关键词： fibrillation sinus rhythm paroxysmal conduction exercise implanted ablation junction repeated

Search for the doubly charmed baryon ■

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Science China(Physics,mechanics & Astronomy) 2020年第2期63卷 8-22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 P.Albicocco J.Albrecht F.Alessio m.a.exa.der A.Alfonso Albero G.Alkhazov P.Alvarez Cartelle A.A.Alves Jr S.Amato Y.Amhis L.An L.Anderlini G.Andreassi m.Andreotti F.Archilli J.Arnau Romeu A.Artamonov m.Artuso K.Arzymatov E.Aslanides m.Atzeni B.Audurier S.Bachmann J.J.Back S.Baker V.Balagura W.Baldini A.Baranov R.J.Barlow S.Barsuk W.Barter m.Bartolini F.Baryshnikov G.Bassi V.Batozskaya B.Batsukh A.Battig V.Battista A.Bay m.Becker F.Bedeschi I.Bediaga A.Beiter L.J.Bel V.Belavin S.Belin N.Beliy V.Bellee K.Belous I.Belyaev G.Bencivenni E.Ben-Haim S.Benson S.Beranek A.Berezhnoy *** D.Berninghoff H.C.Bernstein E.Bertholet A.Bertolin C.Betancourt F.Betti m.O.Bettler Ia.Bezshyiko S.Bhasin J.Bhom m.S.Bieker S.Bifani P.Billoir A.Birnkraut A.Bizzeti m.Bjφrn m.P.Blago T.Blake F.Blanc S.Blusk D.Bobulska V.Bocci O.Boente Garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar S.Borghi m.Borisyak m.Borsato J.T.Borsuk T.J.V.Bowcock C.Bozzi S.Braun A.Brea Rodriguez m.Brodski J.Brodzicka A.Brossa Gonzalo D.Brundu E.Buchanan A.Buonaura C.Burr A.Bursche J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese S.Cali R.Calladine m.Calvi m.Calvo Gomez A.Camboni P.Campana D.H.Campora Perez L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini P.Carniti K.Carvalho Akiba A.Casais Vidal G.Casse m.Cattaneo G.Cavallero R.Cenci J.Cerasoli m.G.Chapman m.Charles Ph.Charpentier G.Chatzikonstantinidis m.Chefdeville V.Chekalina C.Chen S.Chen A.Chernov S.-G.Chitic V.Chobanova m.Chrzaszcz A.Chubykin P.Ciambrone m.F.Cicala X.Cid Vidal G.Ciezarek F.Cindolo 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 A.Comerma-montells A.Contu N.Cooke G.Coombs S.Coquereau G.Corti C.m.Costa Sobral B.Couturier D.C.Craik J.Crkovska A.Crocombe m.Cruz Torres R.Currie C.L.Da Silva E.Dall'Occo J.Dalseno C.D'Ambrosio A.Danilina P.d'Argent A.Davis O.De Aguiar Francisco K.De Bruyn S.De Capua m Centro Brasileiro de Pesquisas Fisicas(CBPF) Rio de JaneiroBrazil Universidade Federal do Rio de Janeiro(UFRJ) Rio de 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) BeijingChina 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 LAL Univ.Paris-SudCNRS/IN2P3Universite Paris-SaclayOrsayFrance LPNHE Sorbonne Universite Paris Diderot Sorbonne Paris Cite CNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-Institut für 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 FrascatiItaly INFN Sezione di Genova GenovaItaly INFN Sezione di milano-Bicocca MilanoItaly INFN Sezione di milano MilanoItaly INFN Sezione di Cagliari MonserratoItaly INFN Sezione di Padova PadovaItaly 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 ScienceKrakowPoland Natio

A search for the doubly charmed baryon ■^+cc is performed through its decay to theΛ^+c K^-π^+ final state,using proton-proton collision data collected with the LHCb detector at centre-of-mass energies of 7,8 and 13 *** data correspond to a total integrated luminosity of 9 fb^-*** significant signal is observed in the mass range from 3.4 to 3.8 GeV/c^*** limits are set at 95%credibility level on the ratio of the ■^+cc production cross-section times the branching fraction to that ofΛ^+c and ■^++cc *** limits are determined as functions of the ■^+cc mass for different lifetime hypotheses,in the rapidity range from 2.0 to 4.5 and the transverse momentum range from 4 to 15 GeV/c.

关键词： charmed baryons limits on production of particles charmed quarks experimental tests

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.a.exa.der 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 Ω^(0)_(bc) and E^(0)_(bc) decaying to Λ^(+)_(c)π^(-) and E^(+)_(c)π^(-)

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Chinese Physics C 2021年第9期45卷 10-21页

作者： R.Aaij C.Abelian Beteta T.Ackernley B.Adeva m.Adinolfi H.Afshamia C.A.Aidala S.Aiola Z.Ajaltouni S.Aka J.Albrecht F.Alessio m.a.exa.der A.Alfonso Albero Z.Aliouche G.Alkhazov P.Alvarez Cartelie 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.Beminghoff 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.Bjorn 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.Camiti 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.Crkovska m.Cruz Torres R.Currie C.L.Da Silva E.Dall'Occo J.Dalseno C.D'Ambrosi Centro Brasileiro de Pesquisas Fisicas(CBPF) Rio de JaneiroBrazil Universidade Federal do Rio de Janeiro(UFRJ) Rio de JaneiroBrazil Center for High Energy Physics Tsinghua UniversityBeijingChina Institute of High Energy Physics(IHEP) BeijingChina School of Physics State Key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University ofChinese Academy of Sciences BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.Savoie mont Blanc CNRSIN2P3-LAPPAnnecyFrance Universite Clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix marseille Univ CNRS/IN2P3CPPMMarseilleFrance Universite Paris-Saclay CNRS/IN2P3IJCLabOrsayFrance Laboratoire Leprince-Ringuet CNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFrance LPNHE Sorbonne UniversiteParis Diderot Sorbonne Paris CiteCNRS/FN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-Institut für Kemphysik(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 FrascatiItaly INFN Sezione di Genova GenovaItaly INFN Sezione di milano MilanoItaly INFN Sezione di milano-Bicocca MilanoItaly INFN Sezione di Cagliari MonserratoItaly Universita degli Studi di Padova Universita e INFNPadovaPadovaItaly INFN Sezione di Pisa PisaItaly INFN Sezione di Roma La Sapienza RomaItaly INFN Sezione di Roma Tor Vergata RomaItaly Nikhef National Institute for Subatomic Physics AmsterdamNetherlands Nikhef National Institute for Subatomic Physics and VU University Amsterdam AmsterdamNetherlands AGH-University of Science and Technology Faculty of Physics and Applied Computer ScienceKr

The first search for the doubly heavyΩ^(0)_(bc)baryon and a search for the E^(0)_(bc)baryon 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 fb^(-1).The baryons are reconstructed via their decays to Λ^(+)_(c)π^(-)and E^(+)_(c)π^(-).No significant excess is fbund for invariant masses between 6700 and 7300 meV/c^(2),in a rapidity range from 2.0 to 4.5 and a transverse momentum range from 2 to 20 meV/*** limits are set on the ratio of the Ω^(0)_(bc)and E^(0)_(bc)production cross-section times the branching fraction to Λ^(+)_(c)π^(-)(E^(+)_(c)π^(-))relative to that of the Λ^(0)_(b)(E^(0)_(b))baryon,for different lifetime hypotheses,at 95%confidence *** upper limits range from 0.5 x 10^(-4)to 2.5 x 10^(-4)for theΩ^(0)_(bc)→Λ^(+)_(c)π^(-)(E^(0)_(bc)→Λ^(+)_(c)π^(-))decay,and from 1.4x 10^(-3)to 6.9 x 10^(-3)for theΩ^(0)_(bc)→E^(+)_(c)π^(-)(E^(0)_(bc)→E^(+)_(c)π^(-))decay,depending on the considered mass and lifetime of theΩ^(0)_(bc)(E^(0)_(bc))baryon.

关键词： B physics quarkonium spectroscopy heavy quark production

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高斯射线束法和理论地震图

地球物理学进展 1988年第4期 66-66页

作者： A.P.Katchalov m.m.popov 冰清

现已提出两种用于计算理论地震图的高斯射线束法,并在模型上进行了检验。第一种方法是基于使用时-空连续高斯射线束,而不是稳定的射线束。第二种是用在一个时间脉冲的光谱密度的极点处的残差和代替傅里叶-频率积分(需要一些辅助的光谱... 详细信息

现已提出两种用于计算理论地震图的高斯射线束法,并在模型上进行了检验。第一种方法是基于使用时-空连续高斯射线束,而不是稳定的射线束。第二种是用在一个时间脉冲的光谱密度的极点处的残差和代替傅里叶-频率积分(需要一些辅助的光谱密度的分析限制)。这两种方法的主要优点如下:(1)可使我们避免计算傅里叶-频率变换;(2)如同高斯射线束法在稳定波场应用一样,这些方法可以克服焦散问题。数值实验的结果证实了这种用于非稳定弹性波场计算的方法的有效性。

关键词：光谱密度理论地震图综合地震图傅里叶