[{"data":1,"prerenderedAt":-1},["ShallowReactive",2],{"_public_publisher_byId_0e586a91-042b-41d0-8604-943ed6669ef2":3,"_public_publication_all{\"sortAscending\":false,\"sortField\":\"updateTime\",\"page\":0,\"size\":10,\"facet\":true,\"searchKey\":\"publisherId:0e586a91-042b-41d0-8604-943ed6669ef2,\"}":19},{"code":4,"data":5,"meta":9},"SUCCESS",{"id":6,"createTime":7,"updateTime":7,"relativeEntities":8,"slug":9,"properties":10,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":16,"manageAffiliations":17,"indexDatabases":18,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},"0e586a91-042b-41d0-8604-943ed6669ef2","2023-12-20T14:43:20.069+00:00",[],null,{"title":11},{"EN":12},"Proceedings of 2002 IEEE 14th International Conference on Dielectric Liquids. ICDL 2002 (Cat. No.02CH37319)","PUBLISHER","PENDING",0,[],[],[],{"meta":20,"data":22},{"total":21},"102",[23,92,136,236,294,353,449,546,604,701],{"id":24,"createTime":25,"updateTime":26,"relativeEntities":27,"slug":28,"properties":29,"entityType":40,"verifyStatus":41,"verifyTime":42,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":44,"fullTextUrl":45,"authors":46,"publicationType":79,"publisherRelationship":80,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"a6d6e026-e2ee-4710-a057-769c7f01cb3b","2023-12-20T14:44:06.316+00:00","2025-01-22T23:54:23.250+00:00",[],"Modeling-of-electrohydrodynamic-flows-and-micro-bubbles-generation-in-dielectric-liquid-by-lattice-Boltzmann-equation-method",{"references":30,"keywords":32,"abstract":34,"title":36,"doi":38},{"VOID":31},"10.1103\u002FPhysRevE.47.1815\nvázquez, 2000, Dynamics of electrobydrodynamic laminar plumes: Scaling analysis. Phys. Fluids, 12, 2809\nkrasuzki, 1966, Breakdown of liquid dielectrics, Proceedings of Royal Society, a294, 393, 10.1098\u002Frspa.1966.0214\n10.1088\u002F0022-3727\u002F28\u002F1\u002F025\n10.1109\u002F14.83669\nmedvedev, 2000, Use of the Lattice Boltzmann Equation Method to Simulate Charge Transfer and Electrohydrodynamic Phenomena in Dielectric Liquids, Proc of the 2nd Int Workshop on Electrical Conduction Convection and Breakdown in Fluids, 60\n10.1146\u002Fannurev.fluid.30.1.329",{"EN":33},"Electrohydrodynamics,Dielectric liquids,Lattice Boltzmann methods,Equations,Fluid flow,Space charge,Charge transfer,Hydrodynamics,Electrodes,Voltage",{"EN":35},"The Lattice Boltzmann Equation (LBE) method was used to simulate a liquid flow with space electric charge. New approach to describe the charge transfer due to convective charge transport was proposed. Simulations of two-dimensional electrohydrodynamic flow showed pulsations caused by the injection of charged blobs and by the hydrodynamic instability of charged jet. Generation and growth of micro-bubbles in strong electric field near the electrode surface was simulated by the LBE method with interparticle interaction. A threshold electric field was found, below that the bubble generation does not occur. At higher fields, the time of bubble development t\u002Fsub d\u002F is approximately inversely proportional to the square of the voltage.",{"EN":37},"Modeling of electrohydrodynamic flows and micro-bubbles generation in dielectric liquid by lattice Boltzmann equation method",{"VOID":39},"10.1109\u002FICDL.2002.1022690","PUBLICATION","VERIFIED","2025-01-22T23:54:23.249+00:00","Auto Verify","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022690\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022690",[47,67],{"id":48,"sortIndex":49,"researcher":9,"roles":50,"affiliations":52,"properties":64},"10a584fe-7343-4c0c-9fa7-460c81b3dce0",1,[51],"AUTHOR",[53],{"id":9,"sortIndex":15,"affiliation":54,"properties":9},{"id":55,"createTime":56,"updateTime":57,"relativeEntities":58,"slug":59,"properties":60,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"a4961381-9684-48a7-99ac-45a3fe08039c","2023-12-07T18:23:50.982+00:00","2024-12-29T08:58:05.248+00:00",[],"Lavrentyev-Institute-of-Hydrodynamics-SB-RAS-Novosibirsk-Russia",{"title":61},{"VI":62},"Lavrentyev Institute of Hydrodynamics SB RAS, Novosibirsk, Russia","AFFILIATION",{"title":65},{"VI":66},"A.L. Kupershtokh",{"id":68,"sortIndex":15,"researcher":9,"roles":69,"affiliations":70,"properties":76},"e30ca833-a2f0-4416-87f1-a9669ba78649",[51],[71],{"id":9,"sortIndex":15,"affiliation":72,"properties":9},{"id":55,"createTime":56,"updateTime":57,"relativeEntities":73,"slug":59,"properties":74,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":75},{"VI":62},{"title":77},{"VI":78},"D.A. 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Asset owners are continually being asked to do more with less. To achieve this monumental task, utility managers need detailed information about the current capability of the transformer, based on its condition (aging and health). Transformer performance assessment (TPA) combines online and offline monitoring to create a total service for both old and new transformers and provides the best possible information about their operation and maintenance needs.",{"EN":104},"Transformer performance assessment",{"VOID":106},"10.1109\u002FICDL.2002.1022758","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022758\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022758",[110],{"id":111,"sortIndex":15,"researcher":9,"roles":112,"affiliations":113,"properties":122},"6f3c96f0-cdd4-4c1b-976c-fcae59e7b22f",[51],[114],{"id":9,"sortIndex":15,"affiliation":115,"properties":9},{"id":116,"createTime":117,"updateTime":117,"relativeEntities":118,"slug":9,"properties":119,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"860dfdc9-5371-4656-9140-9319054d259d","2023-12-20T14:53:28.049+00:00",[],{"title":120},{"VI":121},"VA TECH ELIN Transformatoren, Weiz, Austria",{"title":123},{"VI":124},"A. Garnitschnig",{"url":107,"publisher":126,"properties":133},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":127,"slug":9,"properties":128,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":130,"manageAffiliations":131,"indexDatabases":132,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":129},{"EN":12},[],[],[],{"pages":134},{"VOID":135},"317-320",{"id":137,"createTime":138,"updateTime":139,"relativeEntities":140,"slug":141,"properties":142,"entityType":40,"verifyStatus":41,"verifyTime":139,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":153,"fullTextUrl":154,"authors":155,"publicationType":79,"publisherRelationship":225,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"b016db7c-9b45-4724-ab11-1e3d5e2b2960","2023-12-20T14:53:07.482+00:00","2025-02-09T23:18:18.510+00:00",[],"Measurement-equipment-for-investigation-of-the-influence-of-viscosity-of-dielectric-working-fluids-on-spark-erosion",{"references":143,"keywords":145,"abstract":147,"title":149,"doi":151},{"VOID":144},"wollenberg, 2001, Process energy supply with pulses smaller than 200 ns and their thermal effects on Micro-EDM, 17th Intern Conf on CAPE, 475\nkist, 1999, Streamerausbildung im Mischdielektrikum Isolieröl \u002FTransformerboard, Karlsruhe Univ Diss 1999\nwollenberg, 2000, Scientific report ECOPROD\nschulze, 0, Investigation of the pre-ignition stage in EDM, Proceedings of the 13th ISEM May 9th_11th, 2001, 141",{"EN":146},"Dielectric measurements,Viscosity,Pollution measurement,Pulse measurements,Electric variables measurement,Electrodes,Current measurement,Sparks,Velocity measurement,Pressure measurement",{"EN":148},"In the paper functional goals of the measurement equipment for the investigation of electrical discharges in dielectric working fluids are discussed. Electrical discharges take place at electrode distances smaller than 200 \u002Fspl mu\u002Fm. As an example the influence of the viscosity on the ignition behaviour and on typical phases of the spark erosion are analyzed.",{"EN":150},"Measurement equipment for investigation of the influence of viscosity of dielectric working fluids on spark erosion",{"VOID":152},"10.1109\u002FICDL.2002.1022754","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022754\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022754",[156,172,187,199,212],{"id":157,"sortIndex":158,"researcher":9,"roles":159,"affiliations":160,"properties":169},"cbb5eb13-6708-458b-9483-95b8f7e84dcd",4,[51],[161],{"id":9,"sortIndex":15,"affiliation":162,"properties":9},{"id":163,"createTime":164,"updateTime":164,"relativeEntities":165,"slug":9,"properties":166,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"aaa20f73-d712-4d2f-bd11-0d90664544eb","2023-12-20T14:53:07.513+00:00",[],{"title":167},{"VI":168},"OEL-Held Stuttgar, Germany",{"title":170},{"VI":171},"W. Rehbein",{"id":173,"sortIndex":49,"researcher":9,"roles":174,"affiliations":175,"properties":184},"da1e22c4-2fe3-4d83-9891-89fe9c61ba44",[51],[176],{"id":9,"sortIndex":15,"affiliation":177,"properties":9},{"id":178,"createTime":179,"updateTime":179,"relativeEntities":180,"slug":9,"properties":181,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"5b6c6ed9-ee9e-474e-ae4b-1126fe125112","2023-12-06T07:26:55.121+00:00",[],{"title":182},{"VI":183},"University of Magdeburg, Germany",{"title":185},{"VI":186},"G. Wollenberg",{"id":188,"sortIndex":15,"researcher":9,"roles":189,"affiliations":190,"properties":196},"2965278a-00a8-4f70-b663-307cce7012f3",[51],[191],{"id":9,"sortIndex":15,"affiliation":192,"properties":9},{"id":178,"createTime":179,"updateTime":179,"relativeEntities":193,"slug":9,"properties":194,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":195},{"VI":183},{"title":197},{"VI":198},"H.-P. Schulze",{"id":200,"sortIndex":201,"researcher":9,"roles":202,"affiliations":203,"properties":209},"34406aae-3a87-4e34-9422-a1e2a0130c5e",3,[51],[204],{"id":9,"sortIndex":15,"affiliation":205,"properties":9},{"id":163,"createTime":164,"updateTime":164,"relativeEntities":206,"slug":9,"properties":207,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":208},{"VI":168},{"title":210},{"VI":211},"M. Storr",{"id":213,"sortIndex":214,"researcher":9,"roles":215,"affiliations":216,"properties":222},"07a283f2-46a3-4737-b7fa-f2cd4ea576b8",2,[51],[217],{"id":9,"sortIndex":15,"affiliation":218,"properties":9},{"id":178,"createTime":179,"updateTime":179,"relativeEntities":219,"slug":9,"properties":220,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":221},{"VI":183},{"title":223},{"VI":224},"M. Lauter",{"url":153,"publisher":226,"properties":233},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":227,"slug":9,"properties":228,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":230,"manageAffiliations":231,"indexDatabases":232,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":229},{"EN":12},[],[],[],{"pages":234},{"VOID":235},"301-304",{"id":237,"createTime":238,"updateTime":239,"relativeEntities":240,"slug":241,"properties":242,"entityType":40,"verifyStatus":41,"verifyTime":239,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":253,"fullTextUrl":254,"authors":255,"publicationType":79,"publisherRelationship":283,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"1edaaeae-c7ec-4263-b23a-5c16f9eaf8d9","2023-12-20T14:49:38.908+00:00","2025-02-21T23:13:09.507+00:00",[],"Influence-of-hydrostatic-pressure-on-the-characteristics-of-discharges-propagating-on-solid-liquid-insulating-interfaces-under-AC-and-DC-voltages",{"references":243,"keywords":245,"abstract":247,"title":249,"doi":251},{"VOID":244},"10.1109\u002F57.662781\n10.1063\u002F1.352796\n10.1109\u002FICDL.1996.565420\nbedoui, 2000, Creepage Discharge in Transformer Oil under DC Voltege, IEEE Annual Report of the 2000 Conference on Electrical Insulation and Dielectric Phenomena Victoria British Columbia, 15",{"EN":246},"Solids,Voltage,Electrodes,Power transformer insulation,Dielectric liquids,Surface discharges,Oil insulation,Optical propagation,Safety,Minerals",{"EN":248},"This paper is aimed at the influence of the hydrostatic pressure on the discharge propagating at the liquid\u002Fsolid insulating interfaces under AC and DC voltages using a point-plane electrode arrangement. It is shown that different shapes of creepage discharges and associated currents can be initiated for the same experimental conditions indicating the existence of different propagation modes of discharges. On the other hand, the final length and the number of creepage discharge branches, the corresponding currents and the light emitted are reduced when a hydrostatic pressure is applied; this indicates the implication of gaseous processes in the creepage discharge phenomena. The final length of discharges increases quasi-linearly with the voltage, whatever the type (DC or AC) and polarity of the voltage, and decreases quasi-linearly when the pressure increases.",{"EN":250},"Influence of hydrostatic pressure on the characteristics of discharges propagating on solid\u002Fliquid insulating interfaces under AC and DC voltages",{"VOID":252},"10.1109\u002FICDL.2002.1022731","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022731\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022731",[256,271],{"id":257,"sortIndex":15,"researcher":9,"roles":258,"affiliations":259,"properties":268},"66fc704b-9131-4f6f-baaf-31efcb3132e1",[51],[260],{"id":9,"sortIndex":15,"affiliation":261,"properties":9},{"id":262,"createTime":263,"updateTime":263,"relativeEntities":264,"slug":9,"properties":265,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"4aa74032-642f-40b9-8e98-a1e2cd9ab180","2023-12-20T14:49:38.935+00:00",[],{"title":266},{"VI":267},"Ecole Centrale de Lyon, CEGELY CNRS UMR, Ecully, France",{"title":269},{"VI":270},"A. Beroual",{"id":272,"sortIndex":49,"researcher":9,"roles":273,"affiliations":274,"properties":280},"4ad8d2f1-7638-4f4d-af2b-c270ea2d60b9",[51],[275],{"id":9,"sortIndex":15,"affiliation":276,"properties":9},{"id":262,"createTime":263,"updateTime":263,"relativeEntities":277,"slug":9,"properties":278,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":279},{"VI":267},{"title":281},{"VI":282},"N.K. Bedoui",{"url":253,"publisher":284,"properties":291},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":285,"slug":9,"properties":286,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":288,"manageAffiliations":289,"indexDatabases":290,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":287},{"EN":12},[],[],[],{"pages":292},{"VOID":293},"207-210",{"id":295,"createTime":296,"updateTime":297,"relativeEntities":298,"slug":299,"properties":300,"entityType":40,"verifyStatus":41,"verifyTime":311,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":312,"fullTextUrl":313,"authors":314,"publicationType":79,"publisherRelationship":342,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"d0138889-a293-4c8f-8362-a81f757d3c95","2023-12-20T14:54:00.249+00:00","2024-12-05T22:53:00.024+00:00",[],"Pico-second-time-domain-reflectometry-response-of-a-microstripline-embedded-in-various-liquids",{"references":301,"keywords":303,"abstract":305,"title":307,"doi":309},{"VOID":302},"edwards, 1981, Foundations of Microstrip Circuit Design\n10.1109\u002FEUMA.1975.332206\nsamulon, 1951, Spectrum analysis of transient curves Proc IRE 39, 175\nshannon, 1949, Communication in the presence of noise Proc IRE, 37\n10.1080\u002F02564602.2000.11416927\n1995, HP54753A and HP54754A TDR plug-in modules user's and programmers guides USA\ncole, 1989, J Appl Phys, 66, 10.1063\u002F1.343499\n10.1021\u002Fje980118j",{"EN":304},"Reflectometry,Microstrip,Liquids,Dielectric materials,Chemical technology,Impedance,Optical films,Lamination,Dielectric constant,Dielectric substrates",{"EN":306},"A microstripline having 50 ohms characteristic impedance has been delineated on PCB type FR-4 board material, by using standard three layer dry film lamination and chemical photo-etching technology. The dielectric constant and dissipation factor for FR-4 substrate material is 4.6 and 0.018 at 1 MHz respectively. The fringing fields arising from free end of a microstripline have been employed to observe its free-end-dip liquid response. The microstripline has been vertically dipped in various liquids at different successive lengths. The response due to 40 pico second rise time pulse from free-end-dip of a microstripline in a liquid is observed on the TDR equipment in reflection mode at room temperature. The response waveform obtained is similar to the conventional co-axial transmission line connected to precision SMA cell containing liquid. The data analysis is carried out by standard Fourier transformation techniques. The microstripline of suitable length embedded in a liquid can be used as substitute to the SMA cell to determine the dielectric properties of various liquids.",{"EN":308},"Pico-second time domain reflectometry response of a microstripline embedded in various liquids",{"VOID":310},"10.1109\u002FICDL.2002.1022761","2024-12-05T22:53:00.023+00:00","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022761\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022761",[315,330],{"id":316,"sortIndex":49,"researcher":9,"roles":317,"affiliations":318,"properties":327},"1e4a2fd1-a2a5-439b-8aea-f831e5ab728a",[51],[319],{"id":9,"sortIndex":15,"affiliation":320,"properties":9},{"id":321,"createTime":322,"updateTime":322,"relativeEntities":323,"slug":9,"properties":324,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"18c3e656-164d-4cec-afdf-b3e01c262e3d","2023-12-20T14:54:00.258+00:00",[],{"title":325},{"VI":326},"Department of Computer Science and Information Technology, Aurangabad, India",{"title":328},{"VI":329},"S.C. Mehrotra",{"id":331,"sortIndex":15,"researcher":9,"roles":332,"affiliations":333,"properties":339},"0b8fb24f-e686-4720-8108-690e3331b2ca",[51],[334],{"id":9,"sortIndex":15,"affiliation":335,"properties":9},{"id":321,"createTime":322,"updateTime":322,"relativeEntities":336,"slug":9,"properties":337,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":338},{"VI":326},{"title":340},{"VI":341},"B.R. Sharma",{"url":312,"publisher":343,"properties":350},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":344,"slug":9,"properties":345,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":347,"manageAffiliations":348,"indexDatabases":349,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":346},{"EN":12},[],[],[],{"pages":351},{"VOID":352},"329-332",{"id":354,"createTime":355,"updateTime":356,"relativeEntities":357,"slug":358,"properties":359,"entityType":40,"verifyStatus":41,"verifyTime":356,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":370,"fullTextUrl":371,"authors":372,"publicationType":79,"publisherRelationship":438,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"34f704dd-0cd8-4979-a638-8facb332b2a0","2023-12-20T14:55:30.667+00:00","2025-02-01T22:49:46.229+00:00",[],"Experiments-and-modelling-of-conduction-and-charge-accumulation-in-liquid-crystal-cells",{"references":360,"keywords":362,"abstract":364,"title":366,"doi":368},{"VOID":361},"murakami, 1994, Mol Cryst Liq Cryst\nnaemura, 1997, SID Conf, 199\n10.1080\u002F10587259808045386\n10.1143\u002FJJAP.40.3448\nde vleeschouwer, 2002, Jpn J Appl Phys Part 1, 41\n10.1143\u002FJJAP.40.3272\n10.1149\u002F1.3071413\nverschueren, 2000, IDRC conference, 55\nisraelachvili, 1985, Intermolecular and Surface Forces, 168\nchen, 1999, Eurodisplay Conference, 315",{"EN":363},"Liquid crystals,Liquid crystal displays,Active matrix liquid crystal displays,Voltage measurement,Current measurement,Stress measurement,Impedance measurement,Dielectric constant,Electric variables measurement,Polyimides",{"EN":365},"The combination of different electrical measurements on liquid crystal (display) cells yields a consistent model for charge transport and accumulation. At small timescales (ms) the charge transport is dominated by mobile ions, but on long timescales (hrs) it is demonstrated that the (bulk) generation of extremely. low mobility ions determines the transport. These slow ions accumulate at an ionic double layer at the interface, giving rise to an electric field over the polyimide alignment layer.",{"EN":367},"Experiments and modelling of conduction and charge accumulation in liquid crystal cells",{"VOID":369},"10.1109\u002FICDL.2002.1022773","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022773\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022773",[373,390,402,414,426],{"id":374,"sortIndex":201,"researcher":9,"roles":375,"affiliations":376,"properties":387},"78f680b1-9d07-45f9-bfd9-104ae53e5fbc",[51],[377],{"id":9,"sortIndex":15,"affiliation":378,"properties":9},{"id":379,"createTime":380,"updateTime":381,"relativeEntities":382,"slug":383,"properties":384,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"ec8c3dd3-255f-4bd4-adc2-9e8b546e2052","2023-12-22T19:06:56.158+00:00","2024-12-27T02:23:23.584+00:00",[],"Philips-Research-Laboratories-Eindhoven-Netherlands",{"title":385},{"VI":386},"Philips Research Laboratories, Eindhoven, Netherlands",{"title":388},{"VI":389},"W. Oepts",{"id":391,"sortIndex":49,"researcher":9,"roles":392,"affiliations":393,"properties":399},"ac634112-e554-41a4-926a-b2375175bc6b",[51],[394],{"id":9,"sortIndex":15,"affiliation":395,"properties":9},{"id":379,"createTime":380,"updateTime":381,"relativeEntities":396,"slug":383,"properties":397,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":398},{"VI":386},{"title":400},{"VI":401},"R.A.H. Niessen",{"id":403,"sortIndex":15,"researcher":9,"roles":404,"affiliations":405,"properties":411},"b532131b-5c4c-4c59-bad4-b3d644cdf13c",[51],[406],{"id":9,"sortIndex":15,"affiliation":407,"properties":9},{"id":379,"createTime":380,"updateTime":381,"relativeEntities":408,"slug":383,"properties":409,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":410},{"VI":386},{"title":412},{"VI":413},"A.R.M. Verschueren",{"id":415,"sortIndex":214,"researcher":9,"roles":416,"affiliations":417,"properties":423},"23142207-2d7e-4500-a951-a7ae56f86543",[51],[418],{"id":9,"sortIndex":15,"affiliation":419,"properties":9},{"id":379,"createTime":380,"updateTime":381,"relativeEntities":420,"slug":383,"properties":421,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":422},{"VI":386},{"title":424},{"VI":425},"P.H.L. Notten",{"id":427,"sortIndex":158,"researcher":9,"roles":428,"affiliations":429,"properties":435},"8de68fa1-5d49-4e6a-9bff-a0006f914aa4",[51],[430],{"id":9,"sortIndex":15,"affiliation":431,"properties":9},{"id":379,"createTime":380,"updateTime":381,"relativeEntities":432,"slug":383,"properties":433,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":434},{"VI":386},{"title":436},{"VI":437},"E.M.L. Alexander-Moonen",{"url":370,"publisher":439,"properties":446},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":440,"slug":9,"properties":441,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":443,"manageAffiliations":444,"indexDatabases":445,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":442},{"EN":12},[],[],[],{"pages":447},{"VOID":448},"377-381",{"id":450,"createTime":451,"updateTime":452,"relativeEntities":453,"slug":454,"properties":455,"entityType":40,"verifyStatus":41,"verifyTime":452,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":466,"fullTextUrl":467,"authors":468,"publicationType":79,"publisherRelationship":535,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"38b3300a-c52f-4ee6-8bd7-934665993fbc","2023-12-20T14:47:22.762+00:00","2024-12-19T22:42:42.537+00:00",[],"Electrical-treeing-in-polycrystalline-and-single-crystalline-ices-under-impulse-voltages",{"references":456,"keywords":458,"abstract":460,"title":462,"doi":464},{"VOID":457},"shimizu, 0, Ice as Capacitor Dielectrics, Conf Record of the 1985 Intern Conf on Properties and Applications of Dielectric Materials, 539\n10.1109\u002FTEI.1980.298293\nhikita, 0, Creepage Discharge Propagation on Charged Dielectric Surface in SF6 Gas and Its Optical Observation, Trans IEE Japan, 116 b, 1091\nfarzaneh, 1999, impulse breakdown performance of the ice surface, Proceedings of 11th International Symposium on High-Voltage Engineering (ISH 99), 4, 341\n10.1109\u002F94.311719\nhanaoka, 1996, Characteristics of Creeping Impulse Streamers over the Surface of Oil-Immersed PE Wire, Trans IEE Japan, 116 b, 1091\n10.1049\u002Fcp:19990758\nhobbs, 1974, ICE PHYSICS\n10.1109\u002F14.212248\nmathes, 0, Bridges between Engineering and Science, Cryogenic and Other Dielectric Examples, 1973 Conference on Electrical Insulation and Dielectric Phenomena, 547",{"EN":459},"Ice,Voltage,Permittivity,Dielectrics and electrical insulation,Crystallization,Temperature dependence,Conductivity,Trees - insulation,Dielectric losses,Testing",{"EN":461},"Using two hexagonal H\u002Fsub 2\u002FO ices, polycrystalline and single-crystalline ices, the electrical treeing has been studied under an applied impulse voltage. The crystallinity and temperature of ices play an important role in the events of the treeing. In the single-crystalline ice, the tree in samples at -25\u002Fspl deg\u002FC always progressed along the basal plane of the ice crystal, but at -196\u002Fspl deg\u002FC, it progressed along the C-axis of the crystal. These distinctive patterns on the tree progression were attributed to the crystal-axis dependence of the relative permittivity at each temperature. Intermittent current pulses accompanying the trees were visible in the wave tail of the applied voltage. These current pulses appears to generate by the movement of accumulated charges after the formation of tree channels.",{"EN":463},"Electrical treeing in polycrystalline and single-crystalline ices under impulse voltages",{"VOID":465},"10.1109\u002FICDL.2002.1022717","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022717\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022717",[469,484,499,511,523],{"id":470,"sortIndex":201,"researcher":9,"roles":471,"affiliations":472,"properties":481},"d1752c5d-41f5-4282-bb15-a1d17166a51f",[51],[473],{"id":9,"sortIndex":15,"affiliation":474,"properties":9},{"id":475,"createTime":476,"updateTime":476,"relativeEntities":477,"slug":9,"properties":478,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"bc690bb8-8127-42e4-96b9-19f3b92955d8","2023-12-20T14:47:22.791+00:00",[],{"title":479},{"VI":480},"Fuji EIectric Company Limited, Ichihara, Chiba, Japan",{"title":482},{"VI":483},"Y. Nakagami",{"id":485,"sortIndex":214,"researcher":9,"roles":486,"affiliations":487,"properties":496},"1a5400d3-fdee-4537-acfc-f1bc02ab0a9b",[51],[488],{"id":9,"sortIndex":15,"affiliation":489,"properties":9},{"id":490,"createTime":491,"updateTime":491,"relativeEntities":492,"slug":9,"properties":493,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"17d6a51f-f54c-453e-978f-470ee74beed5","2023-12-20T14:47:22.784+00:00",[],{"title":494},{"VI":495},"Division of Electrical Engineering, Kanazawa Institute of Technology, Nonoichi, Ishikawa, Japan",{"title":497},{"VI":498},"T. Hama",{"id":500,"sortIndex":49,"researcher":9,"roles":501,"affiliations":502,"properties":508},"65ca7c96-6940-405b-b8d5-c6ba46233e6e",[51],[503],{"id":9,"sortIndex":15,"affiliation":504,"properties":9},{"id":490,"createTime":491,"updateTime":491,"relativeEntities":505,"slug":9,"properties":506,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":507},{"VI":495},{"title":509},{"VI":510},"R. Hanaoka",{"id":512,"sortIndex":15,"researcher":9,"roles":513,"affiliations":514,"properties":520},"cfe7146d-07a1-47c7-b355-22ddbceae3ac",[51],[515],{"id":9,"sortIndex":15,"affiliation":516,"properties":9},{"id":490,"createTime":491,"updateTime":491,"relativeEntities":517,"slug":9,"properties":518,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":519},{"VI":495},{"title":521},{"VI":522},"S. Takata",{"id":524,"sortIndex":158,"researcher":9,"roles":525,"affiliations":526,"properties":532},"d1f2d59c-d192-43dd-975a-654449373906",[51],[527],{"id":9,"sortIndex":15,"affiliation":528,"properties":9},{"id":475,"createTime":476,"updateTime":476,"relativeEntities":529,"slug":9,"properties":530,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":531},{"VI":480},{"title":533},{"VI":534},"R. Shimizu",{"url":466,"publisher":536,"properties":543},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":537,"slug":9,"properties":538,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":540,"manageAffiliations":541,"indexDatabases":542,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":539},{"EN":12},[],[],[],{"pages":544},{"VOID":545},"151-154",{"id":547,"createTime":548,"updateTime":549,"relativeEntities":550,"slug":551,"properties":552,"entityType":40,"verifyStatus":41,"verifyTime":549,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":563,"fullTextUrl":564,"authors":565,"publicationType":79,"publisherRelationship":593,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"1a2669b3-60c1-4595-849f-021e1c8bdce3","2023-12-20T14:44:52.033+00:00","2024-12-07T22:39:52.931+00:00",[],"Electrodynamical-currents-in-a-wire-wire-electrode-system",{"references":553,"keywords":555,"abstract":557,"title":559,"doi":561},{"VOID":554},"stishkov, 1986, The ionization-recombination mechanism of charge formation, Reports AS the USSR, 288, 861\nstishkov, 1989, Electrohydrodynamic flows in liquid dielectrics, 17\nstishkov, 1973, Electrohydrodynamical model of conductivity isolated liquids, Electronic Processing of Materials, 62\nostroumov, 1961, About results of measurement of electroconductivity of isolated liquids, Journal of Experimental and Theoretical Physics, 41, 441\natten, 1985, Role of EHD Motion in the Electrical Conduction of Liquids in a Blade-Plane Geometry, IEEE Transactions on Industry Applications, la 21, 709\n10.1109\u002FTEI.1985.348820\nstishkov, 0, Some singularities of EGD-flows in liquid dielectrics, Annual Report of the 2 International Workshop “Electrical Conduction Convection and Breakdown in Fluids”\nstishkov, 2000, The computer analysis of cinematic and dynamic fields of EHD flows, Electronic Processing of Materials",{"EN":556},"Electrodes,Acceleration,Visualization,Wire,Counting circuits,Video recording,Packaging,Conductivity,Liquids,Contamination",{"EN":558},"In the present report, results of computer processing of video recording EHD flows in a symmetric system of electrodes such as two wires are presented. The field of speeds of two-dimensional EHD flows is restored with high accuracy by means of a specially developed package of programs. Visualization of EHD flows represents a challenge, since low conductivity liquids are very sensitive to contamination. Researches have shown that for the visualization of EHD-flows, bubbles can be used. The authors have developed a special computer program for handling videotapes of two-dimensional EHD-flows formed by a wire - wire electrodes. The handling is carried out by means of separate current streamline selection with further recovery of velocity components and acceleration vectors. The results of handling are vector fields of velocities and acceleration, maps of level lines and surface graphs of velocities and acceleration, and also restored streamlines, graphs of acceleration distribution along lines and some integral characteristics, namely consumption of liquid along discretionary selected streamlines of the liquid. In the report, results of the processing of symmetric counter EHD-flows, and also the asymmetrical EHD-flows received by introduction in an initial liquid transformer oil, are given. The comparative analysis of properties of passing and through EHD flows is presented. The analysis of kinematic and dynamic structure of EHD flows, has confirmed the zoned structure of flows, stated earlier, and also in detail has allowed the authors to describe a structure of a zone of recombination and characterise its transformation at the transition from counter EHD flows to through EHD flows. It is shown that through EHD flow is preferable in designing electrohydrodynamic pumps.",{"EN":560},"Electrodynamical currents in a wire-wire electrode system",{"VOID":562},"10.1109\u002FICDL.2002.1022695","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022695\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022695",[566,581],{"id":567,"sortIndex":15,"researcher":9,"roles":568,"affiliations":569,"properties":578},"4f84d6d4-2362-4058-907c-3c4cd335f430",[51],[570],{"id":9,"sortIndex":15,"affiliation":571,"properties":9},{"id":572,"createTime":573,"updateTime":573,"relativeEntities":574,"slug":9,"properties":575,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"38c394ba-3282-4c93-8023-20b67f319101","2023-12-20T14:44:52.045+00:00",[],{"title":576},{"VI":577},"Scientific-Research Institute of Radio physic, Saint Petersburg State University, Saint Petersburg, Russia",{"title":579},{"VI":580},"Y.K. Stishkov",{"id":582,"sortIndex":49,"researcher":9,"roles":583,"affiliations":584,"properties":590},"15abacf7-b872-41cd-9ba3-59f81fe46dc9",[51],[585],{"id":9,"sortIndex":15,"affiliation":586,"properties":9},{"id":572,"createTime":573,"updateTime":573,"relativeEntities":587,"slug":9,"properties":588,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},[],{"title":589},{"VI":577},{"title":591},{"VI":592},"A.V. Buyanov",{"url":563,"publisher":594,"properties":601},{"id":6,"createTime":7,"updateTime":7,"relativeEntities":595,"slug":9,"properties":596,"entityType":13,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"subjectFields":598,"manageAffiliations":599,"indexDatabases":600,"url":9,"thumbnailPath":9,"statistic":9,"gsStatistic":9,"type":9,"analyzePriority":9},[],{"title":597},{"EN":12},[],[],[],{"pages":602},{"VOID":603},"63-66",{"id":605,"createTime":606,"updateTime":607,"relativeEntities":608,"slug":609,"properties":610,"entityType":40,"verifyStatus":41,"verifyTime":607,"verifyNote":43,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15,"primaryUrl":621,"fullTextUrl":622,"authors":623,"publicationType":79,"publisherRelationship":690,"citationCount":9,"citationInfo":9,"publishDate":9,"publishYear":9,"citationAnalyzeStatus":14,"lastCitationAnalyze":9,"indexDatabases":9,"openAccess":9,"references":9,"isForceReanalyzing":91},"a3f19acf-3d6a-49de-974e-786a2203b6d0","2023-12-20T14:54:42.574+00:00","2025-01-07T21:41:12.072+00:00",[],"Study-of-dielectric-relaxation-in-2-4-dimethyl-substituted-pyridine-using-microwave-cavity-spectrometer-and-time-domain-reflectometer",{"references":611,"keywords":613,"abstract":615,"title":617,"doi":619},{"VOID":612},"10.1080\u002F10587250108028692\n10.1103\u002FRevModPhys.18.441\nbladel, 1964, Electromagnetic Fields\ndebye, 1929, Polar Molecules\n10.1039\u002Fft9918701569\npatil, 1998, Sensitive Analysis of Bilinear Calibration Method in Time Domain Reflectometry: 1,2 Propane Diol System, Samyak J Chemistry, 2, 54\nkhirade, 1999, Static Dieelctric Constant and Relaxation Time Measurements on Binary Mixtures of Dimethyl Sulfoxide with Ethanol, 2-Ethoxyethanol, and Propan-1-o1 at 293, 303, 313 And 323 K, J Chemi Engg Data Published on Web, 2.1\n10.1063\u002F1.343499\n10.1109\u002FJRPROC.1949.232969\nsamulon, 1951, spectrum analysis of transient response curves, Proceedings of the IRE, 39, 175, 10.1109\u002FJRPROC.1951.231438\n10.1021\u002Fj100382a014\n10.1088\u002F0022-3735\u002F13\u002F2\u002F001\njohri, 1995, Dielectric Response of Selected Ionic Solutions Using Loaded Microwave Cavity Operating Near 9GHz, 21GHz and 29GHz as a Probe, J Microwave Power and Electromagnetic Energy, 26, 82\njohri, 1995, Dielectric Response and Phase Transition Studies of p-Azoxy Anisol and 1-1 Diacetyl Ferrocene in Pure and. Binary Mixtures, Mol Mat, 5, 63\n10.1080\u002F00319100108031687\n10.1109\u002FICDL.1999.798998\nhill, 1969, Dielectric Properties and Molecular Behaviour\nböttcher, 1978, Theory of Electrical Polarization, 2\njohri, 2000, Study of The Response of Aqueous Solutions of Copper Sulphate Using Microwave Cavity Spectrometer, Phys Chem Liq (In press)\nsingh, 1983, Dielectric Relaxation Studies in Pure Lutidines at Different Microwave Frequencies, Ind J Pure & Appl Phys, 21, 339",{"EN":614},"Electrochemical impedance spectroscopy,Dielectric loss measurement,Dielectric losses,Dielectric measurements,Permittivity measurement,Loss measurement,Time measurement,Temperature,Resonance,Microwave measurements",{"EN":616},"We have used microwave cavity spectrometer and time domain reflectometer for the measurement of permittivity and dielectric loss at different temperatures in 2,4-dimethyl substituted pyridine. The observed data of the width of resonance profile and the shift in the resonance frequency have been analyzed by using Slater perturbation equations useful for cavity spectrometer. The parameters measured from the time domain reflectometer as the function of time at different temperatures have been transformed to obtain permittivity and dielectric loss. The observed values of permittivity and dielectric loss by these two techniques have also been compared. The relaxation time has been evaluated using single relaxation time mechanism and thermodynamical parameters have been determined. This experimental study provides fruitful information about the bulk properties of 2,4-dimethyl substituted pyridine.",{"EN":618},"Study of dielectric relaxation in 2,4-dimethyl substituted pyridine using microwave cavity spectrometer and time domain reflectometer",{"VOID":620},"10.1109\u002FICDL.2002.1022767","https:\u002F\u002Fieeexplore.ieee.org\u002Fabstract\u002Fdocument\u002F1022767\u002F","https:\u002F\u002Fieeexplore.ieee.org\u002Fstamp\u002Fstamp.jsp?tp=&arnumber=1022767",[624,639,654,666,678],{"id":625,"sortIndex":158,"researcher":9,"roles":626,"affiliations":627,"properties":636},"5ba3eb5a-d263-4e55-84b8-d33e770e410b",[51],[628],{"id":9,"sortIndex":15,"affiliation":629,"properties":9},{"id":630,"createTime":631,"updateTime":631,"relativeEntities":632,"slug":9,"properties":633,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"b519a215-af1f-40e4-afe6-66e9d41c42fd","2023-12-20T14:54:50.539+00:00",[],{"title":634},{"VI":635},"Department of Biochemistry, Dr. Virendra Swarup Center of Applied Science and Technology, Kanpur, India",{"title":637},{"VI":638},"S. Saxena",{"id":640,"sortIndex":49,"researcher":9,"roles":641,"affiliations":642,"properties":651},"8e3c5388-3398-4f6f-b8ed-73ee6929e52b",[51],[643],{"id":9,"sortIndex":15,"affiliation":644,"properties":9},{"id":645,"createTime":646,"updateTime":646,"relativeEntities":647,"slug":9,"properties":648,"entityType":63,"verifyStatus":14,"verifyTime":9,"verifyNote":9,"syncStatus":14,"languages":9,"translateLanguages":9,"viewCount":15},"8deca2e2-9a8a-4570-911c-bae3b66ff62f","2024-01-05T20:21:12.767+00:00",[],{"title":649},{"VI":650},"Department of Physics, D.A.V. College, Kanpur, India",{"title":652},{"VI":653},"R. 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