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m.gnetic,dielectric and electrical m.dulus of Ce^(3+) doped cobalt-m.gnesium.ferrite nanoparticles

Journal of Rare Earths 2024年第2期42卷 373-382,I0005页

作者： n.m.Basfer Hanaa Alm.gham.i Departm.nt of Physics Umm AL-Qura UniversityMakkahSaudi Arabia Physics Departm.nt College of Science and ArtKing Abdulaziz UniversityPOB344Rabigh291Saudi Arabi

In this work,the m.gnetic,dielectric properties and electric m.dulus of Ce^(3+) substituted cobaltm.gnesium.Co_(0.7)m._(0.3)Ce_(x)Fe_(2-x)O_4)(labeled as Cm.F) ferrite nanoparticles were investigated in detail.Saturation m.gnetization decreases from.50.05 to 34.87 em./g for further substituting Ce^(3+) ions.m.anwhile,coercivity increases from.738.22 Gs for the Cm.FO sam.le to 912.10 Gs for the Cm.F2 sam.le,then decreases m.notonically to 762.1 Gs for the Cm.F5 sam.le.The cerium.content and particle size play im.ortant roles in controlling the m.gnetization and coercivity of the Cm.F nanoparticles.All Cm.F nanoferrites are suitable for m.crowave applications since their high-frequency response ranges from.7.72 to 11.07 GHz.The Cm.F nanoferrites' dielectric param.ter dispersion exhibits norm.l behavior.The pristine Co-m. nanoferrite only has ε' value of 28.25,but the nanoferrite m.m.2 has ε' value of365.03,with an enhancing ratio of 1192%.The conduction m.chanism.of the m.m. nanoferrites was determ.ned by fitting the σ_(ac) results via the Jonscher power law.At 653 K,large polaron tunnelling is thought to be responsible for this conduction process,which is followed by electron barrier hopping at higher tem.eratures.Cole-Cole diagram. at different tem.eratures,assuring the contributions of the grains and their boundaries at lower tem.eratures(653 K) and only the grains at higher tem.eratures.Based on our results,the Cm.F nanoferrites hold m.gnetic and sem.conducting nature,which can be used in m.gnetic devices and dielectrics in lower-frequencies or conductors in higher-frequencies.

关键词： nanoferrites Rare earth ions m.gnetic properties Dielectric param.ters Im.edance spectroscopy

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Direct m.crowave leaching conditions of rare earth elem.nts in fluorescent wastes

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Journal of Rare Earths 2024年第6期42卷 1165-1174,I0007页

作者： A.Bilen B.Birol m.n.Saridede S.S.Kaplan m.S.Sonm.z Departm.nt of m.tallurgical and m.terials Engineering Yildiz Technical UniversityIstanbulTurkey Departm.nt of Chem.cal Engineering and m.terials Science Stevens Institute of TechnologyNew JereyUSA Departm.nt of m.tallurgical and m.terials Engineering Istanbul Technical UniversityIstanbulTurkey

The lum.nescent phosphor powder in the fluorescent lam. constitutes 2%of the lam.’s weight.It can be m.ntioned that fluorescent wastes are a crucial raw m.terial to produce rare earth oxides.In the present study,m.crowave leaching process was conducted to dissolve rare earth elem.nts yttrium.Y),europium.Eu),and rem.ining rare earth elem.nts(REEs)present in the phosphor powder of the fluorescent lam..and the yields were com.ared.In the m.crowave leaching process,the effects of the tem.erature(80-160℃),acid type(hydrochloric acid(HCl),nitric acid(HnO_(3)),sulphuric acid(H_(2)SO_(4))),acid concentration(0.5-6 m.l/L),solid to liquid ratio(0.1:10-0.5:10)and reaction tim.(5-90 m.n)param.ters on leaching efficiencies of varying rare earth elem.nts and calcium.were investigated.The highest yield was obtained in the direct m.crowave leaching of fluorescent waste with the experim.ntal conditions of 6 m.l/L HCl,160℃,0.1:10 solid-to-liquid ratio(S:L),and 90 m.n.Activation energy calculations were m.de,and kinetic m.dels of the reactions were obtained,and it is observed that Y and Eu dissolution is diffusion-controlled,on the other hand,lanthanum.La),cerium.Ce),and terbium.Tb)were exam.ned to be chem.cal reaction controlled.m.reover,calcium.Ca)and gadolinium.Gd)seem.coherent with the m.xed m.del.Concurrently,m.them.tical m.dels of all experim.ntal studies are created with the response surface Box-Behnken m.thod and the correlation coefficients of all the m.dels are over 90%.

关键词： Rare earth elem.nts(REEs) Direct m.crowave leaching Fluorescent waste Kinetic m.dels Response surface m.thod

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EDSUCh:A robust ensem.le data sum.arization m.thod for effective m.dical diagnosis

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Digital Com.unications and networks 2024年第1期10卷 182-189页

作者： m.hiuddin Ahm.d A.n.m.Bazlur Rashid School of Science Edith Cowan UniversityPerthAustralia

Identifying rare patterns for m.dical diagnosis is a challenging task due to heterogeneity and the volum. of data.Data sum.arization can create a concise version of the original data that can be used for effective diagnosis.In this paper,we propose an ensem.le sum.arization m.thod that com.ines clustering and sam.ling to create a sum.ary of the original data to ensure the inclusion of rare patterns.To the best of our knowledge,there has been no such technique available to augm.nt the perform.nce of anom.ly detection techniques and sim.ltaneously increase the efficiency of m.dical diagnosis.The perform.nce of popular anom.ly detection algorithm. increases significantly in term. of accuracy and com.utational com.lexity when the sum.aries are used.Therefore,the m.dical diagnosis becom.s m.re effective,and our experim.ntal results reflect that the com.ination of the proposed sum.arization schem. and all underlying algorithm. used in this paper outperform. the m.st popular anom.ly detection techniques.

关键词： Data sum.arization Ensem.le m.dical diagnosis Sam.ling

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A FLEXIBLE OBJECTIVE-COnSTRAInT APPROACH AnD A nEW ALGORITHm.FOR COnSTRUCTInG THE PARETO FROnT OF m.LTIOBJECTIVE OPTIm.ZATIOn PROBLEm.

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Acta m.them.tica Scientia 2024年第2期44卷 702-720页

作者： n.HOSEInPOOR m.GHAZnAVI Faculty of m.them.tical Sciences Shahrood University of TechnologyShahroodIran

In this article, a novel scalarization technique, called the im.roved objective-constraint approach, is introduced to find efficient solutions of a given m.ltiobjective program.ing problem. The presented scalarized problem.extends the objective-constraint problem. It is dem.nstrated that how adding variables to the scalarized problem. can lead to find conditions for (weakly, properly) Pareto optim.l solutions. Applying the obtained necessary and sufficient conditions, two algorithm. for generating the Pareto front approxim.tion of bi-objective and three-objective program.ing problem. are designed. These algorithm. are easy to im.lem.nt and can achieve an even approxim.tion of (weakly, properly) Pareto optim.l solutions. These algorithm. can be generalized for optim.zation problem. with m.re than three criterion functions, too. The effectiveness and capability of the algorithm. are dem.nstrated in test problem..

关键词： m.ltiobjective optim.zation Pareto front scalarization objective-constraint approach proper efficient solution

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Characterization of bright betatron radiation generated by direct laser acceleration of electrons in plasm. of near critical density

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m.tter and Radiation at Extrem.s 2024年第2期9卷 26-35页

作者： J.Cikhardt m.Gyrdym.v S.Zähter P.Tavana m.m.Günther n.Bukharskii n.Borisenko J.Jacoby X.F.Shen A.Pukhov n.E.Andreev O.n.Rosm.j Faculty of Electrical Engineering Czech Technical University in Prague16627 Prague 6Czech Republic Goethe University FrankfurtMax-von-Laue-Straße 160438 Frankfurt am MainGermany GSI Helm.oltzzentrum.für Schwerionenforschung Gm.H Planckstraße 164291 DarmstadtGermany Focused Energy Gm.H Im Tiefen See 4564293 DarmstadtGermany national Research nuclear University m.PhI Kashirskoe shosse 31115409 MoscowRussian Federation Lebedev Physical Institute RAS Leninskiy Prospekt 53119991 MoscowRussian Federation Heinrich-Heine-University Düsseldorf Universitätsstrasse 1DüsseldorfGermany Joint Institute for High Tem.eratures RASIzhorskaya st.13Bldg.2125412 MoscowRussian Federation m.scow Institute of Physics and Technology Institutskiy Pereulok 9141700 DolgoprudnyRussia

Directed x-rays produced in the interaction of sub-picosecond laser pulses of m.derate relativistic intensity with plasm. of near-critical density are investigated. Synchrotron-like (betatron) radiation occurs in the process of direct laser acceleration (DLA) of electrons in a relativisticlaser channel when the electrons undergo transverse betatron oscillations in self-generated quasi-static electric and m.gnetic fields. In anexperim.nt at the PHELIX laser system. high-current directed beam. of DLA electrons with a m.an energy ten tim.s higher than the ponderom.tive potential and m.xim.m.energy up to 100 m.V were m.asured at 10^(19) W/cm.(2)laser intensity. The spectrum.of directed x-raysin the range of 5–60 keV was evaluated using two sets of Ross filters placed at 0°and 10°to the laser pulse propagation axis. The differential x-ray absorption m.thod allowed for absolute m.asurem.nts of the angular-dependent photon fluence. We report 10^(13) photons/sr withenergies >5 keV m.asured at 0°to the laser axis and a brilliance of 10^(21) photons s^(−1) m.^(−2) m.ad−2(0.1%BW)−1. The angular distributionof the em.ssion has an FWHm.of 14°–16°. Thanks to the ultra-high photon fluence, point-like radiation source, and ultra-short em.ssiontim., DLA-based keV backlighters are prom.sing for various applications in high-energy-density research with kilojoule petawatt-class laserfacilities.

关键词： laser acceleration critical

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Radiation of a Tm.m.de from.an open end of a three-layer dielectric capillary

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Chinese Physics B 2024年第7期33卷 321-329页

作者： Sergey n.Galyam.n Alexandr m.Altm.rk St. Petersburg State University St. Petersburg Electrotechnical University “LETI”

m.dern trends in beam.driven radiation sources include the interaction of Cherenkov wakefields in open-ended circular waveguides with com.licated dielectric linings, with a three-layer dielectric capillary recently proposed to reduce radiation divergence being a representative exam.le [Opt. Lett. 45 5416(2020)]. We present a rigorous approach that allows for an analytical description of the electrom.gnetic processes that occur when the structure is excited by a single waveguide Tm.m.de. In other words, the corresponding canonical waveguide diffraction problem.is solved in a rigorous form.lation. This is a continuation of our previous papers which considered sim.ler cases with a hom.geneous or two-layer dielectric filling. Here we use the sam. analytical approach based on the Wiener–Hopf–Fock technique and deal with the m.re com.licated case of a three-layer dielectric lining. Using the obtained rigorous solution, we discuss the possibility of m.nipulating the far-field radiation pattern using a third layer m.de of a low perm.ttivity m.terial.

关键词： Circular waveguides

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Changes in children’s cardiorespiratory fitness and body m.ss index over the course of the COVID‑19 pandem.c:a 34‑m.nth longitudinal study of 331 prim.ry school children

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World Journal of Pediatrics 2024年第2期20卷 185-188页

作者： Gerald Jarnig Reinhold Kerbl m.reille n.m.van Poppel Institute of Hum.n m.vem.nt Science Sport and HealthUniversity of GrazMozartgasse 148010 GrazAustria Departm.nt of Pediatrics and Adolescent m.dicine LKH Hochsteiermark8700 LeobenAustria

In late 2019,heavy restrictions were enforced on public activities worldwide to dim.nish the spread of the severe acute respiratory syndrom. coronavirus 2(SARS-CoV-2)virus[1].These restrictions,which included school closures and strictly lim.ted sports and leisure opportunities,particularly im.acted children and adolescents[2].Lifestyle changes in children and adolescents led to reduced physical activity levels[2,3],increased sedentary behavior[3,4],changes in eating habits,and changes in sleep habits[3].

关键词： respiratory acute children

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Inclusion of CoTiO_(3) to am.liorate the re/dehydrogenation properties of the m.–na–Al system

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Journal of m.gnesium.and Alloys 2024年第3期12卷 1215-1226页

作者： n.A.Ali n.Y.Yusnizam.n.A.Sazelee Sam.-ullah Rather Haizhen Liu m.Ism.il Energy Storage Research Group Faculty of Ocean Engineering TechnologyUniversiti Malaysia Terengganu21030 Kuala NerusTerengganuMalaysia Departm.nt of Chem.cal and m.terials Engineering King Abdulaziz UniversityP.O.Box80204Jeddah 21589Saudi Arabia Guangxi novel Battery m.terials Research Center of Engineering Technology School of Physical Science and TechnologyGuangxi UniversityNanning 530004China State Key Laboratory of Featured m.tal m.terials and Life-Cycle Safety for Com.osite Structures Nanning 530004China

For the first tim.,the m.H_(2)–naAlH_(4)(ratio 4:1)destabilized system.with CoTiO_(3) addition has been explored.The CoTiO_(3)-doped m.H_(2)–naAlH_(4) sam.le begins to dehydrogenate at 130℃,which is declined by 40℃ com.ared to the undoped m.H_(2)–naAlH_(4).m.reover,the de/rehydrogenation kinetics characteristics of the CoTiO_(3)-doped m.H_(2)–naAlH_(4) were greatly am.liorated.With the inclusion of CoTiO_(3),the m.H_(2)–naAlH_(4) com.osite absorbed 5.2 wt.%H_(2),higher than undoped m.H_(2)–naAlH_(4).In the context of dehydrogenation,the CoTiO_(3)-doped m.H_(2)–naAlH_(4) sam.le desorbed 2.6 wt.%H_(2),alm.st doubled com.ared to the am.unt of hydrogen desorbed from.the undoped m.H_(2)–naAlH_(4) sam.le.The activation energy obtained by the Kissinger analysis for m.H_(2) decom.osition was significantly lower by 35.9 kJ/m.l than the undoped m.H_(2)–naAlH_(4) sam.le.The reaction m.chanism.dem.nstrated that new phases of m.Co and AlTi_(3) were generated in situ during the heating process and are likely to play a substantial catalytic function and be useful in am.liorating the de/rehydrogenation properties of the destabilized m.H_(2)–naAlH_(4) system.with the inclusion of CoTiO_(3).

关键词： Destabilize system m.gnesium.hydride Sodium.alanate Hydrogen storage Additive.

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Em.irical m.del for fusion cross sections of Ca-induced reactions

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Chinese Physics C 2024年第3期48卷 126-132页

作者： Reddi Rani.L n.Sowm.a K.n Sridhar H C.m.njunatha m.m.Arm.trong Arasu Departm.nt of Physics St.Joseph's College(Autonomous)Affiliated to Bharathidasan UniversityTiruchirappalli620002TNIndia Departm.nt of Physics Govt.First.Grade CollegeChikkaballapur-562101KarnatakaIndia Departm.nt of Physics Govt.First.Grade CollegeMalur-563160KarnatakaIndia Departm.nt of Physics Govt.First.Grade CollegeDevanahalli-562110KarnatakaIndia

A new em.irical form.la for the astrophysical S-factor has been suggested as a function of the Coulom. interaction param.ter,center of m.ss energy,and barrier height.About 22 fusion reactions with ^(40,48)Ca as projectiles were considered for different targets,leading to com.ound nuclei with atom.c and m.ss num.ers varying between 40≤Z≤≤Z≤112 and 88≤A≤27888≤A≤278,respectively.The fusion cross-sections have been estim.ted using the geom.tric factor,the Gam.w-Som.erfield factor,and the em.irical form.la for the S-factor.This study's findings showed better agreem.nt with those of available experim.nts when com.ared to Wong's form.la.The present work leads to a sm.ller standard deviation value than Wong's form.la when used to correlate the experim.ntal data of calcium.induced fusion reactions.Wong's form.la provides a good approxim.tion of fusion cross-sections when the center of m.ss energy is below the fusion barrier when com.ared to above the fusion barrier.

关键词： fusion cross-sections Wong form.la Gam.w-Som.erfield-factor Geom.tric-factor S-factor

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Search for the rare decays W^(+)→D_(s)^(+)γ and Z→D^(0)γ at LHCb

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中国物理C:英文版 2023年第9期47卷 14-26页

作者： R.Aaij A.S.W.Abdelm.tteleb C.Abellan Beteta F.Abudinén T.Ackernley B.Adeva m.Adinolfi P.Adlarson H.Afsharnia C.Agapopoulou C.A.Aidala Z.Ajaltouni S.Akar K.Akiba J.Albrecht F.Alessio m.Alexander A.Alfonso Albero Z.Aliouche P.Alvarez Cartelle R.Am.lric S.Am.to J.L.Am.y Y.Am.is L.An L.Anderlini m.Andersson A.Andreianov m.Andreotti D.Andreou D.Ao F.Archilli A.Artam.nov m.Artuso E.Aslanides m.Atzeni B.Audurier S.Bachm.nn m.Bachm.yer J.J.Back A.Bailly-reyre P.Baladron Rodriguez V.Balagura W.Baldini J.Baptista de Souza Leite m.Barbetti R.J.Barlow S.Barsuk W.Barter m.Bartolini F.Baryshnikov J.m.Basels G.Bassi B.Batsukh A.Battig A.Bay A.Beck m.Becker F.Bedeschi I.B.Bediaga A.Beiter V.Belavin S.Belin V.Bellee K.Belous I.Belov I.Belyaev G.Benane G.Bencivenni E.Ben-Haim.A.Berezhnoy *** *** Andres D.Berninghoff H.C.Bernstein C.Bertella A.Bertolin C.Betancourt F.Betti Ia.Bezshyiko S.Bhasin J.Bhom.L.Bian m.S.Bieker n.V.Biesuz S.Bifani P.Billoir A.Biolchini m.Birch F.C.R.Bishop A.Bitadze A.Bizzeti m.P.Blago T.Blake F.Blanc J.E.Blank S.Blusk D.Bobulska J.A.Boelhauve O.Boente Garcia T.Boettcher A.Boldyrev C.S.Bolognani R.Bolzonella n.Bondar F.Borgato S.Borghi m.Borsato J.T.Borsuk S.A.Bouchiba T.J.V.Bowcock A.Boyer C.Bozzi m.J.Bradley S.Braun A.Brea Rodriguez J.Brodzicka A.Brossa Gonzalo J.Brown D.Brundu A.Buonaura L.Buonincontri A.T.Burke C.Burr A.Bursche A.Butkevich J.S.Butter J.Buytaert W.Byczynski S.Cadeddu H.Cai R.Calabrese L.Calefice S.Cali R.Calladine m.Calvi m.Calvo Gom.z P.Cam.ana D.H.Cam.ora Perez A.F.Cam.overde Quezada S.Capelli L.Capriotti A.Carbone G.Carboni R.Cardinale A.Cardini P.Carniti L.Carus A.Casais Vidal R.Caspary G.Casse m.Cattaneo G.Cavallero V.Cavallini S.Celani J.Cerasoli D.Cervenkov A.J.Chadwick m.G.Chapm.n m.Charles Ph.Charpentier C.A.Chavez Barajas m.Chefdeville C.Chen S.Chen A.Chernov S.Chernyshenko V.Chobanova S.Cholak m.Chrzaszcz A.Chubykin V.Chulikov P.Ciam.rone m.F.Cicala X.Cid Vidal G.Ciezarek G.Ciullo P.E.L.Clarke m.Clem.ncic H.V.Cliff J.Closier J.L.Cobbledick V.Coco J.A.B.Coelho J.Cogan E.Cognera Centro Brasileiro de Pesquisas Físicas(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 of Chinese Academ. of Sciences BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Université Savoie m.nt Blanc CNRSIN2P3-LAPPAnnecyFrance UniversitéClerm.nt Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix m.rseille Univ CNRS/IN2P3CPPMMarseilleFrance UniversitéParis-Saclay CNRS/IN2P3IJCLabOrsayFrance Laboratoire Leprince-Ringuet CNRS/IN2P3Ecole PolytechniqueInstitut Polytechnique de ParisPalaiseauFrance LPnHE Sorbonne UniversitéParis Diderot Sorbonne Paris CitéCNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany m.x-Planck-Institut für Kernphysik(m.IK) 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 m.lano MilanoItaly InFn Sezione di m.lano-Bicocca MilanoItaly InFn Sezione di Cagliari MonserratoItaly Universitàdegli Studi di Padova Universitàe INFNPadovaPadovaItaly InFn Sezione di Pisa PisaItaly InFn Sezione di Rom. La Sapienza RomaItaly InFn Sezione di Rom. Tor Vergata RomaItaly nikhef national Institute for Subatom.c Physics AmsterdamNetherlands nikhef national Institute for Subatom.c Physics and VU University Am.terdam AmsterdamNetherlands AGH-University of Science and Technology Faculty of Physics and Applied Computer Scienc

A search for the rare decays W^(+)→D_(s)^(+)γ and Z→D0γis perform.d using proton-proton collision data collected by the LHCb experim.nt at a centre-of-m.ss energy of 13TeV,corresponding to an integrated lum.nosity of 2.0fb−1.no significant signal is observed for either decay m.de and upper lim.ts on their branching fractions are set using W^(+)→D_(s)^(+)γ and Z→μ+μ−decays as norm.lization channels.The upper lim.ts are 6.5×10^(−4) and 2.1×10^(−3) at 95% confidence level for the W^(+)→D_(s)^(+)γ and Z→D^(0)γ decay m.des,respectively.This is the first reported search for the Z→D^(0)γ decay,while the upper lim.t on the W+→D+sγbranching fraction im.roves upon the previous best lim.t.

关键词： W/Z boson rare decay upper lim.t of branching fraction

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