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Zollikar, D. E. Cox, J. M. Tranquade, and G. Shirane,Phys. Rev. B 38, 6575 (1988).\nT. Kajitani, K. Kusaba, M. Kikuchi, Y. Syono, and M. Hirabayashi,Jpn. J. Appl. Phys. 27, L354 (1988).\nY. Xu, M. Suenega, J. Tafto, R. L. Sabatini, A. R. Moodenbaugh, and P. Zolliker,Phys. Rev. B. 39, 6667 (1989).\nB. D. Dunlap, J. D. Jorgensen, C. Segre, A. E. Dwight, J. L. Matykiewicz, H. Lee, W. Peng, and C. W. Kimball,Physica C 158, 387 (1989).\nR. Sonntag, D. Hohlwein, A. Hoser, W. Prandl, W. Schafer, R. Kiemel, S. Kemmler-Sack, S. Losch, M. Schlichenmaier, and A. W. Hewat,Physica C 159, 141 (1989).\nF. Bridges, J. B. Boyce, T. Claeson, T. H. Geballe, and J. M. Tarascon,Phys. Rev. B 39, 11603 (1989).\nY. Xu, R. L. Sabatini, A. R. Moodenbaugh, Y. Zhu, S-G. Shyu, M. Suenaga, K. W. Dennis, and R. W. McCallum,Physica C 169, 205 (1990).\nJ. A. Hriljac, A. R. Moodenbaugh, and Y. Xu,Physica C 219, 315 (1994).\nE. Suard, A. Maignan, V. Caignaert, and B. Raveau,Physica C 200, 43 (1992).\nH. Renevier, J. L. Hodeau, M. Marezio, and A. Santoro,Physica C 220, 143 (1994).\nN. H. Anderson, J. V. Andersen, L. Borjesson, R. Hadfield, M. Kakihana, R. McGreevy, O. G. Mourtisen, and H. F. Poulsen,J. Alloys Cpnd. 195, 327 (1993).\nP. F. Miceli, J. M. Tarascon, L. H. Greene, F. J. Rotella, and J. D. Jorgensen,Phys. Rev. B 37, 5932 (1988).\nM. G. Smith, J. B. Goodenough, A. Manthiram, R. D. Taylor, and H. Oesterreicher,Phys. Rev. B 46, 3041 (1992).\nE. Suard, V. Caignaert, A. Maignan, F. Bouree, and B. Raveau,Physica C 210, 164 (1993).\nD. B. Wiles and R. A. Young,J. Appl. Crystallogr. 14, 149 (1981).\nA. Sequeira,Physica B 174, 311 (1991).\nR. J. Cava, A. W. Hewat, E. A. Hewat, B. Batlogg, M. Marezio, K. M. Rabe, J. J. Krajewsk, W. F. Peck, Jr., and L. W. Rupp,Physica C 165, 419 (1990).\nJ. D. Jorgensen, B. W. Veal, A. P. Paulikas, L. J. Nowicki, G. W. Crabtree, H. Claus, and W. K. Kwock.Phys. Rev. B 41, 1863 (1990).\nH. Renevier, J. L. Hodeau, M. Marezio, A. Fontaine, A. Michalowicz, and G. Tourillon,Phys. Rev. B 47, 11398 (1993).\nV. P. S. Awana and A. V. Narlikar,Phys. Rev. B 49, 6353 (1994).\nC. Greaves and P. R. Slater,Supercond. Sci. Technol. 2, 5 (1989).\nI. D. Brown and D. Altermatt,Acta Cryst. B 41, 244 (1985).",{"EN":228},"The results of a systematic powder neutron study on Y1−x\nCaxBa2Cu3−y\nCo\n                  y\n                O7±δ for A (x=y=0), B (x=0;y=0.2), C (x= 0;y=0.4), D (x=y=0.2), and E (x=y=0.4) are investigated with a view to understanding the relation between the structural parameters and superconductivity. Rietveld refinements of the structures show that: (a) Co substitutes at the chain Cu(1) sites only, except for sample E, where the presence of a minor amount of Co at the planar Cu(2) site cannot be ruled out; (b) Co substitution reduced thec-parameter, which is reduced even further upon substitution of Ca at the Y-sites; (c) the occupancy factors of the chain O(1) site indicate an average coordination of 4.8 and 5.1 for Co for samples B and C, but only 4 for D and E; (d) Cu\u002FCo(1) atoms for B and C display large thermal parameters, suggesting a displacement from their ideal centrosymmetric location; (e) the apical Cu(1)-O(4) bond lengthens upon substitution of Co in samples B and C but undergoes shortening upon substitution of Ca in the case of samples D and E. The apical Cu(2)-O(4) bond, on the other hand, shows just the opposite trend; (f) samples D and E show a reduction in the separation of CuO2 layers and their oxygen content; and (e) the bond valence of the Cu(2) ion shows the lowest value of 2.127 for the nonsuperconducting sample C.",{"EN":230},"Neutron structural investigations of Y1−x CaxBa2Cu3−y Co y O7±δ",{"VOID":232},"10.1007\u002FBF00732380","PUBLICATION","VERIFIED","Auto Verify","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002FBF00732380",[238,254,269,282,295,308],{"id":239,"sortIndex":21,"researcher":20,"roles":240,"affiliations":242,"properties":251},"1e9c844e-355e-4159-9fa8-e90182fc963f",[241],"AUTHOR",[243],{"id":20,"sortIndex":21,"affiliation":244,"properties":20},{"id":245,"createTime":246,"updateTime":246,"relativeEntities":247,"slug":20,"properties":248,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"c33b20c8-3e74-4469-a569-e145829b5622","2024-01-09T21:29:54.589+00:00",[],{"title":249},{"VI":250},"Solid State Physics Division, Bhabha Atomic Research Centre, Bombay, India",{"title":252},{"VI":253},"Rajni Sharma",{"id":255,"sortIndex":181,"researcher":20,"roles":256,"affiliations":257,"properties":266},"3cc3cfc7-fa4d-418c-bbee-f46cc9325794",[241],[258],{"id":20,"sortIndex":21,"affiliation":259,"properties":20},{"id":260,"createTime":261,"updateTime":261,"relativeEntities":262,"slug":20,"properties":263,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"b401493d-2bf4-4445-bf13-fb88964e9ef1","2024-01-13T18:50:51.027+00:00",[],{"title":264},{"VI":265},"Chemistry Division, Bhabha Atomic Research Centre, Bombay, India",{"title":267},{"VI":268},"R. Ganguly",{"id":270,"sortIndex":271,"researcher":20,"roles":272,"affiliations":273,"properties":279},"12d0fbb4-7966-497d-b22d-2285fe263e64",4,[241],[274],{"id":20,"sortIndex":21,"affiliation":275,"properties":20},{"id":260,"createTime":261,"updateTime":261,"relativeEntities":276,"slug":20,"properties":277,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},[],{"title":278},{"VI":265},{"title":280},{"VI":281},"J. V. Yakhmi",{"id":283,"sortIndex":284,"researcher":20,"roles":285,"affiliations":286,"properties":292},"508acf67-0848-436c-a088-0cf6af58283b",2,[241],[287],{"id":20,"sortIndex":21,"affiliation":288,"properties":20},{"id":245,"createTime":246,"updateTime":246,"relativeEntities":289,"slug":20,"properties":290,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},[],{"title":291},{"VI":250},{"title":293},{"VI":294},"H. Rajagopal",{"id":296,"sortIndex":297,"researcher":20,"roles":298,"affiliations":299,"properties":305},"730e06ed-a227-447d-8779-97439f506789",5,[241],[300],{"id":20,"sortIndex":21,"affiliation":301,"properties":20},{"id":245,"createTime":246,"updateTime":246,"relativeEntities":302,"slug":20,"properties":303,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},[],{"title":304},{"VI":250},{"title":306},{"VI":307},"B. A. Dasannnacharya",{"id":309,"sortIndex":310,"researcher":20,"roles":311,"affiliations":312,"properties":318},"73005654-85b0-456f-99f9-9fdc3230bf0e",3,[241],[313],{"id":20,"sortIndex":21,"affiliation":314,"properties":20},{"id":245,"createTime":246,"updateTime":246,"relativeEntities":315,"slug":20,"properties":316,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},[],{"title":317},{"VI":250},{"title":319},{"VI":320},"A. Sequeira","ARTICLE",{"url":236,"publisher":323,"properties":351},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":324,"slug":10,"properties":325,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":329,"manageAffiliations":330,"indexDatabases":331,"url":20,"thumbnailPath":20,"statistic":346,"gsStatistic":20,"type":20,"analyzePriority":20},[],{"issn":326,"eissn":327,"title":328},{"VOID":13},{"VOID":15},{"EN":17},[],[],[332,339],{"id":84,"indexDatabase":333,"url":99,"indexYears":20,"academicFieldIds":338,"indexDatabaseRanking":20},{"id":86,"createTime":87,"updateTime":88,"relativeEntities":334,"label":335,"description":336,"key":95,"publicationTags":337,"standard":20},[],{"EN":91,"VI":91},{"VI":93,"EN":94},[97,98],[101],{"id":64,"indexDatabase":340,"url":77,"indexYears":78,"academicFieldIds":345,"indexDatabaseRanking":82},{"id":66,"createTime":67,"updateTime":68,"relativeEntities":341,"label":342,"description":343,"key":74,"publicationTags":344,"standard":20},[],{"EN":71,"VI":71},{"EN":71,"VI":73},[76],[80,81],{"impactFactor":21,"impactFactorByYear":347,"i10Index":116,"i10IndexLast5Year":117,"totalPublication":118,"totalPublicationByYear":348,"totalCitation":154,"totalCitationByYear":349,"totalCitationPerPublication":182,"totalCitationPerPublicationByYear":350,"hindexLast5Year":123,"hindex":123},{"1995":104,"1996":21,"2012":105,"2013":106,"2014":107,"2015":108,"2016":109,"2017":110,"2018":110,"2019":111,"2020":112,"2021":113,"2022":114,"2023":115},{"1988":120,"1989":121,"1990":122,"1991":123,"1992":124,"1993":125,"1994":126,"1995":127,"1996":128,"1997":129,"1998":130,"1999":131,"2000":132,"2001":133,"2002":134,"2003":135,"2004":136,"2005":137,"2006":138,"2007":139,"2008":136,"2009":140,"2010":141,"2011":142,"2012":143,"2013":144,"2014":145,"2015":146,"2016":147,"2017":148,"2018":149,"2019":150,"2020":144,"2021":151,"2022":152,"2023":126,"2024":153},{"1988":156,"1989":157,"1990":158,"1991":159,"1992":160,"1993":122,"1994":161,"1995":162,"1996":159,"1997":163,"2004":164,"2005":165,"2006":166,"2007":161,"2008":167,"2009":168,"2010":169,"2011":170,"2012":171,"2013":172,"2014":173,"2015":174,"2016":175,"2017":176,"2018":177,"2019":178,"2020":179,"2021":180,"2022":140,"2023":137,"2024":181},{"1988":184,"1989":185,"1990":186,"1991":187,"1992":188,"1993":189,"1994":190,"1995":191,"1996":192,"1997":193,"2004":194,"2005":195,"2006":110,"2007":196,"2008":197,"2009":198,"2010":199,"2011":200,"2012":201,"2013":202,"2014":203,"2015":204,"2016":205,"2017":206,"2018":207,"2019":208,"2020":209,"2021":210,"2022":211,"2023":212,"2024":213},{"volume":352,"pages":354},{"VOID":353},"8",{"VOID":355},"271-277","1995-04-01",1995,false,{"id":360,"createTime":361,"updateTime":362,"relativeEntities":363,"slug":364,"properties":365,"entityType":233,"verifyStatus":234,"verifyTime":362,"verifyNote":235,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":374,"fullTextUrl":20,"authors":375,"publicationType":321,"publisherRelationship":408,"citationCount":20,"citationInfo":20,"publishDate":442,"publishYear":443,"citationAnalyzeStatus":19,"lastCitationAnalyze":20,"indexDatabases":20,"openAccess":20,"references":20,"isForceReanalyzing":358},"69fa34bd-2835-4bff-88d7-1ac1f4d61485","2023-12-31T09:24:31.836+00:00","2024-12-14T23:59:43.297+00:00",[],"Metamagnetic-Phase-Transitions-in-La1-x-Nd-x-Mn2Si2",{"references":366,"abstract":368,"title":370,"doi":372},{"VOID":367},"Duman, E., Acet, M., Dincer, I., Elmali, A., Elerman, Y.: Competing magnetic interactions in rare-earth manganese silicides and germanides. J. Magn. Magn. Mater. 309, 40–53 (2007)\nMoriya, T., Usami, K.: Coexistence of ferro- and antiferromagnetism and, phase transitions in itinerant electron systems. Solid State Commun. 23, 935–938 (1977)\nBrabers, J.H.V.J., Nolten, A.J., Kayzel, F., Lenczowski, S.H.J., Buschow, K.H.J., De Boer, F.R.: Strong Mn–Mn distance dependence of the Mn interlayer coupling in SmMn2Ge2-related compounds and its role in magnetic phase transitions. Phys. Rev. B 50(22), 16410–16417 (1994)\nBrabers, J.H.V.J., Buschow, K.H.J., De Boer, F.R.: Field-induced first-order antiferromagnetic–ferromagnetic transitions in RMn2Ge2 compounds and their relation to the magnetostriction of the Mn sublattice. Phys. Rev. B 59(14), 9314–9323 (1999)\nDincer, I., Elerman, Y., Elmali, A., Ehrenberg, H., André, G.: Neutron diffraction study of the La1−x Pr x Mn2Si2 (x=0.4, 0.7 and 1) compounds and the general description of the magnetic behavior of Mn in RMn2Ge2 and RMn2Si2. J. Magn. Magn. Mater. 313(2), 342–353 (2007)",{"EN":369},"Experimental measurements for the magnetization at various temperatures are analyzed using a mean field model for the purely ferromagnetic spin configuration near the metamagnetic phase transitions in La1−x\n                Nd\n                  x\n                Mn2Si2 (x=0.3) at a constant magnetic field (50 mT). By fitting the temperature dependence of the magnetization from the free energy in the mean field model to the experimental data for this compound, the coefficients in the free energy expansion are determined. Our analysis of the magnetization describes a first-order character of the metamagnetic transition in La1−x\n                Nd\n                  x\n                Mn2Si2 (x=0) on the basis of the mean field model studied here.",{"EN":371},"Metamagnetic Phase Transitions in La1−x Nd x Mn2Si2",{"VOID":373},"10.1007\u002Fs10948-012-1916-3","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs10948-012-1916-3",[376,391],{"id":377,"sortIndex":181,"researcher":20,"roles":378,"affiliations":379,"properties":388},"093de300-e488-46b0-ac76-6a3bb696e8d8",[241],[380],{"id":20,"sortIndex":21,"affiliation":381,"properties":20},{"id":382,"createTime":383,"updateTime":383,"relativeEntities":384,"slug":20,"properties":385,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"b31964f9-afb0-418c-bfc9-5c61ec0b9d63","2023-12-31T09:24:31.864+00:00",[],{"title":386},{"VI":387},"Department of Physics, Middle East Technical University, Ankara, Turkey",{"title":389},{"VI":390},"H. Yurtseven",{"id":392,"sortIndex":21,"researcher":20,"roles":393,"affiliations":394,"properties":405},"3040c69b-277d-45f6-baf2-dba60ed81fdc",[241],[395],{"id":20,"sortIndex":21,"affiliation":396,"properties":20},{"id":397,"createTime":398,"updateTime":399,"relativeEntities":400,"slug":401,"properties":402,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"04a52964-5570-4032-9845-3821885cf5ec","2023-12-31T09:24:31.846+00:00","2025-06-11T17:53:35.207+00:00",[],"Department-of-Engineering-Physics-Faculty-of-Engineering-University-of-Ankara-Ankara-Turkey",{"title":403},{"VI":404},"Department of Engineering Physics, Faculty of Engineering, University of Ankara, Ankara, Turkey",{"title":406},{"VI":407},"B. 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H., Clark, S. R., Jaksch, D.: EPJ Quantum Technology 1, 1 (2014)\nBuluta, I., Nori, F.: Science 326, 108 (2009)\nJaksch, D., Bruder, C., Cirac, J., Gardiner, C., Zoller, P.: Phys. Rev. Lett. 81, 3108 (1998)\nGreiner, M., Mandel, O., Esslinger, T., Hänsch, T. W., Bloch, I.: Nature 415, 39 (2002)\nSpielman, I. B., Phillips, W. D., Porto, J. V.: Phys. Rev. Lett. 98, 080404 (2007)\nSpielman, I. B., Phillips, W. D., Porto, J. V.: Phys. Rev. Lett. 100, 120402 (2008)\nBloch, I., Jean, D., Wilhelm, Z.: Rev. Mod. Phys. 80, 885 (2008)\nJiang, L., Rey, A. M., Romero-isart, O., García-ripoll, J. J., Sanpera, A., Lukin, M. D.: Phys. Rev. A 79, 022309 (2009)\nKnap, M., Arrigoni, E., Linden, W. V. D.: Phys. Rev. B 81, 024301 (2010)\nZhang, X. h., Kou, S. p.: Int. J. Mod. Phys. B 27(4), 1250214 (2013)\nCapogrosso-Sansone, B., Soyler, S. G., Prokof’ev, N., Svistunov, B.: Phys. Rev. A 77, 015602 (2008)\nFisher, M. P. A., Weichman, P. B., Grinstein, G., Fisher, D. S.: Phys. Rev. B 40, 546 (1989)\nNikolaev, S. V., Ovchinnikov, S. G.: J. Exp. Theor. Phys. 111(4), 635 (2010)\nHubbard, J.: Proceedings of the Royal Society A Mathematical. Phys. Eng. Sci. 276, 238 (1963)\nOvchinnikov, S., Val’kov, V.: Hubbard Operators in the Theory of Strongly Correlated Electrons. Imperial College Press, London (2004)\nElstner, N., Monien, H.: Phys. Rev. B 59(9), 12184 (1999)",{"EN":454},"We study the two-dimensional ultracold Bose gas in optical lattice. We use cluster perturbation theory based on Hubbard X-operators to calculate the spectral function and phase diagram of Bose-Hubbard model which is minimal model to describe behavior of ultracold gases in optical lattices. We have analyzed spectral properties of spinless bosons in a square lattice taking into account the short-range correlation.",{"EN":456},"Spectral Properties of the Bose-Hubbard Model Within the Cluster Perturbation Theory in X-Operators Representation",{"VOID":458},"10.1007\u002Fs10948-016-3781-y","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs10948-016-3781-y",[461,490,502],{"id":462,"sortIndex":181,"researcher":20,"roles":463,"affiliations":464,"properties":487},"4561732f-f033-4936-9649-f1682736cf05",[241],[465,477],{"id":466,"sortIndex":181,"affiliation":467,"properties":476},"e4d33b86-4b84-4aa7-812b-fcb5651d8dc0",{"id":468,"createTime":469,"updateTime":470,"relativeEntities":471,"slug":472,"properties":473,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"06d75008-7b02-4909-9d2a-c6dd58da6370","2023-12-11T05:06:37.346+00:00","2025-06-11T19:53:57.958+00:00",[],"Kirensky-Institute-of-Physics-Siberian-Branch-Russian-Academy-of-Sciences-Krasnoyarsk-Russia",{"title":474},{"VI":475},"Kirensky Institute of Physics, Siberian Branch, Russian Academy of Sciences, Krasnoyarsk, Russia",{},{"id":20,"sortIndex":21,"affiliation":478,"properties":20},{"id":479,"createTime":480,"updateTime":481,"relativeEntities":482,"slug":483,"properties":484,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"1606e79a-73a4-42bc-a42b-2129d2f6683c","2023-12-28T20:52:41.058+00:00","2024-12-10T23:03:20.523+00:00",[],"Siberian-Federal-University-Krasnoyarsk-Russia",{"title":485},{"VI":486},"Siberian Federal University, Krasnoyarsk, Russia",{"title":488},{"VI":489},"Sergey Nikolaev",{"id":491,"sortIndex":21,"researcher":20,"roles":492,"affiliations":493,"properties":499},"f0e47ef6-b8a8-4ae1-b273-9e1e1eb64894",[241],[494],{"id":20,"sortIndex":21,"affiliation":495,"properties":20},{"id":479,"createTime":480,"updateTime":481,"relativeEntities":496,"slug":483,"properties":497,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},[],{"title":498},{"VI":486},{"title":500},{"VI":501},"Kirill 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Nagarajan, C. Mazumdar, Z. Hossain, S. K. Dhar, K. V. Gopalkrishnan, L. C. Gupta, C. Godart, B. D. Padalia, and R. Vijayaraghavan, Phys. Rev. Lett. 72, 274 (1994).\nR. J. Cava, H. Takagi, H. W. Zandbergen, J. J. Krajewski, W. F. Peck, T. Siegrist, B. Batlogg, R. B. van Dover, R. J. Felder, K. Mizuhashi, J. O. Lee, H. Eisaki, and S. Uchida, Nature 367, 252 (1994).\nL. C. Gupta, R. Nagarajan, C. Godart, S. K. Dhar, C. Mazumdar, Z. Hossain, C. Levy-Clement, B. D. Padalia, and R. Vijayaraghavan, Physica C 150, 235 (1994).\nT. Siegrist, H. W. Zandbergen, R. J. Cava, J. J. Krajewski and W. F. Peck, Nature 367, 254 (1994).\nZ. Hossain, L. C. Gupta, R. Nagarajan, S. K. Dhar, C. Godart and R. Vijayaraghavan, Physica B 223-224, 99 (1996).\nJ. Cava, H. Takagi, B. Batlogg, H. W. Zandbergen, J. J. Krajewski, W. F. Peck, Van R Bover, R. J. Felder, T. Siegrist, K. Mizuhashi, J. O. Lee, H. Eisaki, S. A. Carter, and S. Uchida, Nature 367, 146 (1994).\nK. D. D. Rathnayaka, A. K. Bhatnagar, A. Parasiris, D. G. Naugle, P. C. Canfield, and B. K. Cho, Phys. Rev. B 55, 8506 (1997).\nM. Xu, P. C. Canfield, J. E. Ostenson, D. K. Finnemore, B. K. Cho, Z. R. Wang and D. C. Johnston, Physica C 227, 321 (1994).\nC. Mazumdar, Z. Hossain, S. Radha, A. K. Nigam, R. Nagarajan, L. C. Gupta, C. Godart, B. D. Padalia, G. Chandra, and R. Vijayaraghavan, Physica B 223-224, 102 (1996).\nR. M. Kadam, M. D. Sastry, Z Hossain, C. Mazumdar, R. Nagarajan, L. C. Gupta, C. Godart, and R. Vijayaraghavan, Physica C 232, 359 (1994).\nY. Y. Xue, Y. Cao, R. L. Meng, V. Kinalidis, and C. W. Chu, Physica C 227, 63 (1994).\nS. B. Roy, Z. Hossain, A. K. Pradhan, C. Mazumdar, P. Chaddah, R. Nagarajan, C. Godart, and L. C. Gupta, Physica C 228, 319 (1994).\nX. Z. Zhou, H. P. Kunkel, P. A. Stampe, J. A. Cowen and G. Williams, Physica C 251, 183 (1995).\nK. Ghosh, S. Ramakrishnan, A. K. Grover, G. Chandra, T. V. Chandrasekhar Rao, P. K. Mishra, G. Ravikumar, and V. C. Sahni, Phys. Rev. B 52 68; (1995). Physica B 223-224, 109 (1996).\nS. B. Roy, Z. Hossain, A. K. Pradhan, P. Chaddah, R. Nagarajan, and L. C. Gupta, Physica C 256, 90 (1996).\nU. Yaron, P. L. Gammel, A. P. Ramirez, D. A. Huse, D. J. Canfield, K. Mortensen, and M. R. Eskildsen, Nature 382, 236 (1996).\nA. Andreone, F. Fontana, M. Iavarone, R. Vaglio, F. Canepa, P. Manfrinetti, and A. Palenzona, Physica C 251, 379 (1995).\nN. Khare, A. K. Gupta, S. Khare, L. C. Gupta, R. Nagarajan, Z. Hossain and R. Vijayaraghavan, Appl. Phys. Lett. 69, 148 (1996).\nA. K. Gupta, S. K. Agarwal, B. Jayaram, A. Gupta, and A. V. Narlikar, Pramana-J Phys. 28, L705 (1987).\nJ. T. Chen., L. E. Wegner, C. J. McEwanand, and E. M. Logothetis, Phys. Rev. Lett. 58, 1972 (1987).\nC. M. Pegrum, G. B. Donaldson, A. Carr, and A. Hendry, Appl. Phys. Lett. 51, (1987) 1364; C. M. Pegrum, J. B. Buckley, and M. Odehnal, IEEE Trans MAG 25, 872 (1989).\nN. Khare, A. K. Gupta, S. K. Arora, V. S. Tomar, and V. N. Ojha, Pramana-J Phys. 35, L415 (1990); 35, 243 (1990).\nN. Khare, A. K. Gupta, S. Chaudhry, and V. S. Tomar, Solid State Commun. 76, 29 (1990).\nN. Khare, A. K. Gupta, A. K. Saxena, K. K. Verma, and O. N. Srivastava, Supercon. Sci. Technol. 7, 402 (1994).\nN. Khare, A. K. Gupta, H. K. Singh, and O. N. Srivastava, Supercond. Sci. Technol. 11, 517 (1998).\nC. Godart, L. C. Gupta, R. Nagarajan, S. K. Dhar, H. Noel, M. Potel, C. Mazumdar, Z. Hossain, C. Levy-Clement, G. Schriffmacher, B. D. Padalia, and R. Vijayaraghavan, Phys. Rev. B 51, 489 (1995).\nK. K. Likharev, Introduction to the Dynamics of Josephson Junctions and Circuits. Gordon and Breach, New York (1986) Chap. 14, p. 471.",{"EN":567},"This paper reports observation of rf-SQUID effect due to natural grain boundary junctions in YNi2B2C (T\nc ∼ 15.5 K), ErNi2B2C (T\nc ∼ 11.5 K, T\nN ∼ 6.5 K), and DyNi2B2C (T\nc ∼ 6.5 K, T\nN ∼ 11K), LuNi2B2C (T\nc ∼ 16.5 K) and YPd5B3C0.35 (T\nc ∼ 23 K) bulk borocarbide superconductors. The observation of rf-SQUID effect due to natural grain boundary junctions in all the five borocarbide superconductors clearly indicates that natural grain boundary junctions in these superconductors behave as Josephson junctions, and this behavior of natural grain boundary junctions in the quaternary borocarbides appear to be universal in this class of superconductors. Observation of rf-SQUID effect in magnetic borocarbide superconductors (ErNi2B2C and DyNi2B2C) at 4.2 K also indicates that antiferromagnetic ordering does not destroy SQUID effect, as T\nN > 4.2 K in both cases. Rapid increase in flux noise due to thermally activated flux hopping has been observed in all the SQUIDs as temperature approaches T\nc.",{"EN":569},"rf-SQUID Effect in Bulk Quaternary Borocarbide Superconductors",{"VOID":571},"10.1023\u002FA:1026418709682","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1023\u002FA:1026418709682",[574,589,606,618,630],{"id":575,"sortIndex":21,"researcher":20,"roles":576,"affiliations":577,"properties":586},"7fef5f6e-4744-41e2-870d-e7756906ffd3",[241],[578],{"id":20,"sortIndex":21,"affiliation":579,"properties":20},{"id":580,"createTime":581,"updateTime":581,"relativeEntities":582,"slug":20,"properties":583,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"186d295c-42bf-4d67-a6d9-a045c35ef65e","2024-01-04T11:34:40.787+00:00",[],{"title":584},{"VI":585},"National Physical Laboratory, New Delhi, India",{"title":587},{"VI":588},"Neeraj Khare",{"id":590,"sortIndex":284,"researcher":20,"roles":591,"affiliations":592,"properties":603},"bab334e6-660d-4758-a73b-84d702e86b13",[241],[593],{"id":20,"sortIndex":21,"affiliation":594,"properties":20},{"id":595,"createTime":596,"updateTime":597,"relativeEntities":598,"slug":599,"properties":600,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"184736c2-805e-4b53-96ae-e8ef41ef9b53","2024-01-11T20:10:41.057+00:00","2025-02-03T22:19:26.273+00:00",[],"Tata-Institute-of-Fundamental-Research-Bombay-India",{"title":601},{"VI":602},"Tata Institute of Fundamental Research, Bombay, India",{"title":604},{"VI":605},"Z. 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B 86, 134402 (2012)\nSchaffry, M., Filidou, V., Karlen, S.D., Gauger, E.M., Benjamin, S.C., Anderson, H.L., Ardavan, A., Briggs, G.A.D., Maeda, K., Henbest, K.B., Giustino, F., Morton, J.J.L., Lovett, B.W.: Phys. Rev. Lett. 104, 200501 (2010)",{"EN":691},"Using a full ab initio method, based on quantum chemical wave function methods with the inclusion of spin-orbit coupling and a static external magnetic field, we investigate the laser-induced, ultrafast spin transfer in the three-magnetic-center cluster Ni3Na2 under various static distortions. In this manuscript we study and identify three important factors, i.e. the interatomic distances, the number of bridging atoms, and the spin direction, in order to obtain a series of rules of thumb. It is found that the spin transfer between Ni atoms mainly depends on the number of Na atoms and the spin direction on the Ni atoms, and only the scenarios between Ni2 and Ni3 atoms with the spin direction at Ni3 atom along the x and z axes can be achieved.",{"EN":693},"First-Principles Study of the Ultrafast, Laser-Induced Spin Transferability in the Multi-center Magnetic Cluster 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Phys. Today 63, 38–43 (2010)\nBussmann-Holder, A., Keller, H.: High-temperature superconductors: underlying physics and applications. Z. Naturforsch. 75, 3–14 (2020)\nPureur, P., Menegotto Costa, R.: Fluctuation phenomena in high temperature superconductors. In: Ausloos, M., Varlamov, A.A. (eds.) NATO-ASI Series 3, vol. 32, pp. 259–269. Kluwer, Netherlands, Dordrecht (1997)\nAslamazov, L.G., Larkin, A.I.: The influence of fluctuation pairing of electrons on the conductivity of normal metal. Phys. Lett. 26A, 238–239 (1968)\nLobb, C.J.: Critical fluctuations in high-Tc superconductors. Phys. Rev. B 36, 3930–3932 (1987)\nBardeen, J., Cooper, L.N., Schrieffer, J.R.: Theory of Superconductivity. Phys. Rev. 108, 1175–1204 (1957)\nPureur, P., Menegotto Costa, R., Rodrigues, P., Jr., Schaf, J., Kunzler, J.V.: Critical and Gaussian conductivity fluctuations in YBa2cu3O7–δ. Phys. Rev. B 47, 11420–11425 (1993)\nRoa-Rojas, J., Menegotto Costa, R., Pureur, P., Prieto, P.: Pairing transition, coherence transition, and the irreversibility line in granular GdBa2cu3O7–δ. Phys. Rev. B 61, 12457–12462 (2001)\nJurelo, A.R., Abrego Castillo, I., Roa-Rojas, J., Ferreira, L.M., Ghivelder, L., Pureur, P., Rodrigues, P., Jr.: Coherence transition in granular high temperature superconductors. Physica C 311, 133–139 (1999)\nRosenblatt, J.: Percolation, localization and superconductivity. In: Goldman, A.M., Wolf, S.A. (eds) NATO ASI Series, p. 431, Plenum, New York (1984).\nRojas Sarmiento, M.P., Uribe Laverde, M.A., Vera López, E., Landínez Téllez, D.A., Roa-Rojas, J.: Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7–δ material. Phys. B 398, 360–363 (2007)\nLarkin, A., Varlamov, A.: Theory of fluctuations in superconductors. Oxford Science Publications, New York (2005)\nKouvel, J.S., Fisher, M.E.: Detailed magnetic behavior of nickel. Near its Curie Point. Phys. Rev. A 163, 1626–1632 (1964).\nGinzburg, V.L.: Several remarks on second-order phase transitions in microscopy theory of ferroelectrics. Fiz. Tverd. Tela 2, 2031 (1960) [Sov. Phys. Solid State 2, 1824 (1961)].\nRoa-Rojas, J., Jurelo, A.R., Menegotto Costa, R., Mendonça Ferreira, L., Pureur, P., Orlando, M.T.D., Prieto, P., Nieva, G.: Fluctuation conductivity and the dynamical universality class of the superconducting transition in high-Tc cuprates. Physica C 341–348, 1911–2012 (2000).\nHohenberg, P.C., Halperin, B.I.: Theory of dynamic critical phenomena. Rev. Mod. Phys. 49, 435–479 (1977)\nLidmar, J., Wallin, M., Wengel, C., Girvin, S.M., Young, A.P.: Dynamical universality classes of the superconducting phase transition. Phys. Rev. B 58, 2827–2833 (1998)\nRoa-Rojas, J., Prieto, P., Pureur, P.: Hall conductivity fluctuations in epitaxial YBa2cu3O7–δ thin films. Mod. Phys. Lett. B 15, 1117–1129 (2001)\nChar, K., Kapitulnik, A.: Fluctuation conductivity in inhomogeneous superconductors. Z. Phys. B 72, 253–259 (1988)\nTsuchiya, Y., Awaji, S., Watanabe, K., Miura, S., Ichino, Y., Yoshida, Y., Matsumoto, K.: Delocalization of vortex in SmBa2Cu3O7−δ superconducting films with BaHfO3 nano-rods. J. Appl. Phys. 120, 103902 (2016).\nFaley, M.I., Liu, Y., Dunin-Borkowski, R.E.: Titanium nitride as a new prospective material for NanoSQUIDs and superconducting nanobridge electronics. Nanomaterials 11, 466 (2021)\nMendonça Ferreira, L., Pureur, P., Borges, H.A., Lejay, P.: Effects of pressure on the fluctuation conductivity of YBa2Cu3O7.δ Phys. Rev. B 69, 212505 (2004).\nVarshney, D., Singh, R.K., Shah, S.: Coherence lengths and magnetic penetration depths in YBa2Cu3O7 and YBa2Cu4O8 superconductors. J. Supercond. 9, 629–635 (1996)\nGasparov, V.A., Mkrtchyan, M.R., Obolensky, M.A., Bondarenko, A.V.: Anomalous temperature dependence of the electromagnetic penetration depth of Y1Ba2Cu3O7–δ crystals. Physica C 231, 197–206 (1994)\nMorris, D.E., Nickel, J.H., Wei, J.Y.T., Asmar, N.G., Scott, J.S., Scheven, U.M., Hultgren, C.T., Marketz, A.G., Post, J.E., Heaney, P.J., Veblen, D.R., Hazen, R.M.: Eight new high-temperature superconductors with the 1:2:4 structure. Phys. Rev. B 39, 7347–7350 (1989)\nHarshman, D.R., Aeppli, G., Ansaldo, E.J., Batlogg, B., Brewer, J.H., Carclan, J.F., Cava, R.J., Celio, M., Chaklader, A.C.D., Hardy, W.N., Kreitzman, S.R., Luke, G.M., Noakes, D.R., Senba, M.: Temperature dependence of the magnetic penetration depth in the high-Tc superconductor Ba2YCu3O9−δ: evidence for conventional s-wave pairing. Phys. Rev. B 36, 2386–2389 (1987)\nEscribe-Filippini, C., Konate, K., Buder, R., Marcus, J., Schlenker, C.: High Tc superconducting properties of SmBa2Cu3O7−x: thermal properties. Physica C 153–155, 1030–1031 (1988)\nPlackowski, T., Wtosewicz, D., Sutkowski, C., Rogacki, K.: Negative charge carriers in the 90 K plateau of REBa2Cu3O7−δ. Physica C 244, 54–62 (1995)\nKoblischka, M.R., Koblischka-Veneva, A., Zeng, X.L., Hannachi, E., Slimani, Y.: Microstructure and fluctuation-induced conductivity analysis of Bi2Sr2CaCu2O8+d (Bi-2212) nanowire fabrics. Curr. Comput.-Aided Drug Des. 10, 986 (2020)\nEagles, D.M.: Specific heats and thermodynamic critical fields in Zn-doped YBa2Cu3O7-x according to an induced-pairing model. Physica C 211, 319–328 (1993)\nJoshi, K.R., Nusran, N.M., Tanatar, M.A., Cho, K., Meier, W.R., Bud’ko, S.L., Canfield, P.C., Prozorov, R.: Measuring the lower critical field of superconductors using nitrogen-vacancy centers in diamond optical magnetometry. Phys. Rev. Appl. 11, 014035 (2019).\nMaple, M.B., Dalichaouch, Y., Ferreira, J.M., Hake, R.R., Lee, B.W., Neumeier, J.J., Torikachvili, M.S., Yang, K.N., Zhou, H.: Phys. B 148, 155 (1987)",{"EN":875},"Synthesis of the SmBa2Cu3O7–δ superconducting material by the standard solid-state reaction is reported. DC resistivity measurements were performed to analyse the conductivity excess close to the superconducting transition. The fluctuation analysis was performed by the method of logarithmic temperature derivative of the paraconductivity. A bulk Tc = 93.004 K was determined through the extrapolation of the genuinely critical regime, which is explained from the dynamical scaling theory. The correlations of the critical exponents with the dimensionality of the fluctuation system for each Gaussian regime were performed by using the Aslamazov–Larkin theory. From the analysis, the occurrence of Gaussian-like fluctuations associated to dimensional d = 3 and d = 2 pairing regimes and fluctuation developing in fractal topologies with d = 2.6 and d = 1.3 are established. The coherence length, the Ginzburg number, the jump in the specific heat δc at T = Tc, the penetration depth λ(0), the critical magnetic fields Bc1(T) and Bc2(T) and the critical current density Jc(0) were theoretically determined for this superconducting material. Results largely agree with experimental reports for RBa2Cu3O7–δ (R = Rare Earth elements) and YBa2Cu3O7–δ superconductors.",{"EN":877},"Superconducting Critical Parameter Calculation from the Analysis of the Paraconductivity in SmBa2Cu3O7–δ",{"VOID":879},"10.1007\u002Fs10948-021-06019-1","https:\u002F\u002Flink.springer.com\u002F10.1007\u002Fs10948-021-06019-1",[882,897,909,921,933],{"id":883,"sortIndex":284,"researcher":20,"roles":884,"affiliations":885,"properties":894},"81fafa19-a1ef-4791-986c-1efb8e68931a",[241],[886],{"id":20,"sortIndex":21,"affiliation":887,"properties":20},{"id":888,"createTime":889,"updateTime":889,"relativeEntities":890,"slug":20,"properties":891,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"b9d0a404-52de-4d31-ac5b-4deb418452f9","2023-12-07T04:38:47.335+00:00",[],{"title":892},{"VI":893},"Grupo de Física de Nuevos Materiales, Departamento de Física, Universidad Nacional de Colombia, Bogotá, Colombia",{"title":895},{"VI":896},"L. 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Mater. 30, 718 (2018)\nWang, Y.G., Zhang, H., Zhu, J.L.: Adv. Mater. 32, 1905007 (2019)\nChern, M.Y., Vennos, D.A., Disalvo, F.J.: J. Solid State Chem. 96, 415 (1992)\nArca, E., Lany, S., Perkins, J.: J. Am. Chem. Soc. 140, 4293 (2018)\nTan, S.G., Gao, C.H., Yuan, H., Wu, J.P., Wang, C.: J. Solid State Chem. 302, 122389 (2021)\nStoiber, D., Niewa, R.: Z. Anorg. Allg. Chem. 645, 329 (2019)\nNuss, J., Mühle, C., Hayama, K.: Acta Cryst. B 71, 300 (2015)\nGäbler, F., Kirchner, M., Schnelle, W.: Z. Anorg. Allg. Chem. 630, 2292 (2004)\nSun, Y., Chen, X.Q., Yunoki, S.: Phys. Rev. Lett. 105, 216406 (2010)\nGoh, W.F., Pickett, W.E.: Phys. Rev. B 98, 125147 (2018)\nMa, H., Zhang, X.D., Wang, F.: Vacuum 191, 110410 (2021)\nKrimi, Y.E., Masrour, R., Jabar, A.: J. Mol. Graph. Model. 114, 108165 (2022)\nPan, Y., Jing, C.: Ceram. Int. 45, 21373 (2019)\nPan, Y.: Int. J. Hydrogen Energy 44, 18153 (2019)\nDai, J., Ju, M.G., Ma, L., Zeng, X.C.: J. Phys. Chem. C 123, 6363 (2019)\nChaouche, Y.: Bull. Mater. Sci. 44, 111 (2021)\nChi, E.O., Kim, W.S., Hur, N.H., Jung, D.: Solid State Commun. 121, 309 (2002)\nHeinselman, K.N., Lany, S., Perkins, J.D., Talley, K.R.: Chem. Mater. 31, 8717 (2019)\nSreedevi, P.D., Ravindran, P., Vidy, R.: Materials Today: Proceedings 8, 294 (2019)\nMochizuki, Y., Sung, H.J., Takahashi, A.: Phys. Rev. Mater. 4, 044601 (2020)\nRani, U., Kamlesh, P.K., Shukla, A., Verma, A.S.: J. Solid State Chem. 300, 122246 (2021)\nAmara, K., Zemouli, M., Elkeurti, M.: J. Alloy. Compd. 576, 398 (2013)\nSegall, M.D., Lindan, P.J.D., Probert, M.J.: J. Phys. Condens. Matter 14, 2717 (2002)\nZhong, H.X., Feng, C.B., Wang, H.: Appl. Mater. Interfaces 13, 48516 (2021)\nBilal, M., Ahmad, I., Aliabad, H.A.R., Asadabadi, S.J.: Comput. Mater. Sci. 85, 310 (2014)\nShein, I.R., Ivanovskii, A.L.: J. Solid State Chem. 177, 61 (2004)\nKhandy, S.A., Islam, I., Kaur, K.: Results Phys. 17, 103112 (2020)\nVoigt, W.: Ann. Phys. Chem. 274, 573 (1889)\nReuss, A.: ZAMM-Z Angew. Math. Me. 9, 49 (1929)\nRani, U., Soni, Y., Kamlesh, P.K.: Int. J. Energy Res. 45, 13442 (2021)\nWang, J.F., Fu, X.N., Wang, J.T.: Chin. Phys. B 26, 106301 (2017)\nKuma, S., Woldemariam, M.M.: Adv. Condens. Matter Phys. 2019, 3176148 (2019)\nSun, Z., Li, S., Ahuja, R., Schneider, J.M.: Solid State Commun. 129, 589 (2004)\nPugh, S.F.: Philos. Mag. 45, 823 (1954)\nMedkour, Y., Roumili, A., Maouche, D.: J. Alloy. Compd. 541, 75 (2012)\nVaitheeswaran, G., Kanchana, V., Svane, A., Delin, A.: J. Phys. Condens. Matter 19, 326214 (2007)\nVaitheeswaran, G., Kanchana, V., Kumar, R.S.: Phys. Rev. B 76, 014107 (2007)\nSattar, M.A., Benkraouda, M., Amrane, N.: Physica E 118, 113885 (2020)\nAtanelov, J., Mohn, P.: Comput. Mater. Sci. 117, 380 (2016)\nGolafroozShahri, S., Roknabadi, M.R., Shahtahmasebi, N., Behdani, M.: J. Magn. Magn. Mater. 420, 56 (2016)\nPushpa, R., Daniel, D., Butt, D.P.: Solid State Ionics 249, 184 (2013)\nBai, A.M., Zhao, S.F., Chen, J.Y.: J. Nanomater. 2014, 509408 (2014)\nPark, J.H., Lee, Y.A., Lee, J.H., Yoon, H.: J. Asian. Ceram. Soc. 8, 519 (2020)\nMarugata, S., Kagi, H., Ijichi, Y.: J. Solid. State. Chem. 312, 123258 (2022)\nShi, K.W., Sun, Y., Colin, C.V.: Phys. Rev. B 97, 054110 (2018)",{"EN":991},"In this work, the antiperovskite semiconductor compounds Mg3XN (X = P, As, Sb, Bi) are investigated using the first-principles calculations. The structural, electronic, optical, and elastic properties of the Mg3XN compounds are studied in detail. Meanwhile, the magnetism is introduced by doping Mn element in Mg3XN compounds. Mg3XN compounds are semiconductors with direct band gap from the analysis of electronic properties. In addition, the values of band gap decrease with the increasing of atomic number of X atoms. The results of elastic parameters show that the values of bulk (91.27 GPa) and shear (76.14 GPa) modulus of Mg3PN are the largest in the Mg3XN compounds. For the velocity of sound in different directions of Mg3XN compounds, the Mg3PN has the maximum average velocity of sound, which implies that the bonding strength of Mg3PN is at maximum. Moreover, the changes of bulk modulus, shear modulus, and Young’s modulus under different pressure are explored. By substituting Mg atoms with Mn atoms, the chemical formula of Mg3XN compounds is updated to Mg2.5Mn0.5XN. The conclusions of the formation enthalpy and magnetic properties of Mg2.5Mn0.5XN compounds confirm that the possibility of Mg3XN compounds becomes photovoltaic materials. We hope that the present work can provide some reference for the application of Mg3XN compounds.",{"EN":993},"Potential Antiperovskite Semiconductor Compounds Mg3XN (X = P, As, Sb, Bi): the First-Principles Study",{"VOID":995},"10.1007\u002Fs10948-022-06373-8","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs10948-022-06373-8",[998,1013,1025,1040,1052],{"id":999,"sortIndex":181,"researcher":20,"roles":1000,"affiliations":1001,"properties":1010},"4c5d1f86-709a-4054-90d2-4fc2b4c142d2",[241],[1002],{"id":20,"sortIndex":21,"affiliation":1003,"properties":20},{"id":1004,"createTime":1005,"updateTime":1005,"relativeEntities":1006,"slug":20,"properties":1007,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"1560eef2-a966-4a76-87ce-542c5bfc8139","2023-12-20T04:52:18.008+00:00",[],{"title":1008},{"VI":1009},"School of Science, Shenyang University of Technology, Shenyang, 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Science Technol. 17, 377 (2002)\nEkicibil, A.: Solid State Sci. 14, 1486–1491 (2012)\nAkyol, M., Ekicibil, A., Kiymac, K.: J. Supercond. Nov. Magn. 26, 3257–3262 (2013)\nNakamura, S.: Science 281, 956 (1998)\nMirkin, C.A.: Science 286, 2095 (1999)\nSharma, V.K., Xalxo, R., Varma, G.D.: Cryst. Res. Technol. 42, 34–38 (2007)\nHuang, G.J., Wang, J.B., Zhong, X.L., Zhou, G.C., Yan, H.L.: J. Mater. Sci. 42, 6464–6468 (2007)\nDietl, T., Ohno, H., Matsukura, F., Cibert, J., Ferrand, D.: Science 287, 1019–1022 (2000)\nSato, K., Katayama, H.: Jpn. J. Appl. Phys. Part 2 40, L334–L336 (2001)\nSato, K., Katayama- Yoshida, H.: Jpn. J. Appl. Phys. Part 2 39, L555–L558 (2000)\nVenkatesan, M., Stamenov, P., Dorneles, L.S., Gunning, R.D., Bernoux, B., Coey, J.M.D.: Appl. Phys. Lett. 90, 242508 (2007)\nYu, M., Qiu, H., Chen, X., Liu, H., Wang, M.: Physica B 404, 1829–1834 (2009)\nIshizumi, A., Kanemitsu, Y.: Appl. Phys. Lett. 86, 253106 (2005)\nZhou, Z., Komori, T., Yoshino, M., Morinaga, M., Matsunami, N., Koizumi, A., Takeda, Y.: Appl. Phys. Lett. 86, 041107 (2005)\nDhar, S., Brandt, O., Ramsteiner, M., Sapega, V.K., Ploog, K.H.: Phys. Rev. Lett. 94, 037205 (2005)\nMa, X.: Thin Solid Films 520, 5752–5755 (2012)\nPotzger, K., Zhou, S.Q., Eichhorn, F., Helm, M., Skorupa, W., Mücklich, A., Fassbender, J., Herrmannsdörfer, T., Bianchi, A.: J. Appl. Phys. 99, 063906 (2006)\nUngureanu, M., Schmidt, H., Xu, Q., Wenckstern, H., Spemann, D., Hochmuth, H., Lorenz, M., Grundmann, M.: Superlattices Microstruct 42, 231 (2007)\nOzgur, U., Aliov, Ya. I., Liu, C., Teke, A., Reshchikov, M.A., Dogan, S., Avrutin, V., Cho, S.J., Markoc, H.: Appl. Phys. Rev. 98, 041301 (2005)\nMandal, S.K., Das, A.K., Nath, T.K.: J. Appl. Phys. 104315, 1–8 (2006)\nDas, J., Mishra, D.K., Sahu, D.R., Roul, B.K.: Phys. B 407, 3575–3579 (2012)\nSrinivasan, G., Seehra, M.S.: Phys. Rev. B 28, 1470 (1983)\nAkyol, M., Ekicibil, A., Firat, T., Kiymac, K., Supercond, J.: Nov. Magn. 26, 2439–2445 (2013)\nChaillout, C., Alario- Franco, M.A., Cappani, J.J., Chenavas, J., Strobel, P., Marezio, M.: Sol. State Comm. 65, 283 (1988)\nSarsari, I.A., Salamati, H., Kameli, P., Ravazi, F.S., Supercond, J.: Nov. Magn. 24, 2293–2298 (2011)\nMandal, S.K., Nath, T.K. Thin Solid Films 515, 2535–2541 (2006)",{"EN":1107},"We have worked on the structural and magnetic properties of Zn0.99−xMn0.01Gd\n                  x\n                O\n                  δ\n                (for x = 0.02, 0.03, and 0.04) compounds prepared by using a sol–gel method. The x-ray diffraction, scanning electron microscopy, and energy dispersive x-ray spectroscopy were used to understand the structural properties of the samples. We observed that co-substitution of Mn (1 %) and Gd (2–4 %) into the ZnO does not change the hexagonal structure. Scanning electron microscope (SEM) images show us that the grain size decreases with the increasing amount of the Gd into the ZnO matrix. The magnetic properties of the samples have been investigated by using magnetic hysteresis and DC susceptibility measurements. The ZMG1 sample shows a weak ferromagnetic behavior at room temperature, whereas the ZMG2 and ZMG3 samples exhibit a paramagnetic nature. Furthermore, it is also found that the magnetizations of the samples decrease with increasing Gd content in the ZnMnO system due to the enhancing interaction between Gd 3+ ions. We summarize that the co-substitution of Mn and Gd into the ZnO generates a room-temperature ferromagnetism, but it still needs more work to obtain strong and high coercivity magnetic loops for applications.",{"EN":1109},"Effects of Mn and Gd Co-substituted into ZnO on Structural and Magnetic Properties",{"VOID":1111},"10.1007\u002Fs10948-014-2640-y","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs10948-014-2640-y",[1114,1129,1145,1157,1169,1181],{"id":1115,"sortIndex":310,"researcher":20,"roles":1116,"affiliations":1117,"properties":1126},"2f5092d5-1578-4ce6-bead-f8d928ada7e9",[241],[1118],{"id":20,"sortIndex":21,"affiliation":1119,"properties":20},{"id":1120,"createTime":1121,"updateTime":1121,"relativeEntities":1122,"slug":20,"properties":1123,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"c17a8734-657d-45aa-9647-a7db7e7ae2b0","2024-01-04T16:09:35.859+00:00",[],{"title":1124},{"VI":1125},"Department of Physics, Faculty of Sciences and Letters, Adıyaman University, Adıyaman, Turkey",{"title":1127},{"VI":1128},"Ali Osman 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B., Ulrichs, H., Garbs, F., Muenzenberg, M.: The building blocks of magnonics. Phys. Rep. 507, 107–136 (2011)\nKhitun, A., Bao, M., Wang, K.L.: Magnonic logic circuits. J. Phys. D 43, 264005 (2010)\nKajiwara, Y., Harii, K., Takahashi, S., Ohe, J., Uchida, K., Mizuguchi, M., Umezawa, H., Kawai, H., Ando, K., Takanashi, K., Maekawa, S., Saitoh, E.: Transmission of electrical signals by spin-wave interconversion in a magnetic insulator. Nature 464, 262–266 (2010)\nSerga, A.A., Chumak, A.V., Hillebrands, B.: YIG magnonics. J. Phys. D 43, 264002 (2010)\nTomasello, R., Martinez, E., Zivieri, R., Torres, L., Carpentieri, M., Finocchio, G.: A strategy for the design of skyrmion racetrack memories. Sci. Rep. 4, 6784 (2014)\nChumak, A.V., Vasyuchka, V.I., Serga, A.A., Hillebrands, B.: Magnon spintronics. Nat. Phys. 11, 453–461 (2015)\nKozhevnikov, A., Gertz, F., Dudko, G., Filimonov, Y., Khitun, A.: Pattern recognition with magnonic holographic memory device. Appl. Phys. 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Nano Lett. 17, 2703–2712 (2017)\nEmori, S., Bauer, U., Ahn, S.M., Martinez, E., Beach, G.S.D.: Current-driven dynamics of chiral ferromagnetic domain walls. Nat. Mater. 12, 611–616 (2013)\nThiaville, A., Rohart, S., Jue, E., Cros, V., Fert, A.: Dynamics of Dzyaloshinskii domain walls in ultrathin magnetic films. Europhys. Lett. 100, 57002 (2012)\nHu, B., Wang, X.R.: Instability of Walker propagating domain wall in magnetic nanowires. Phys. Rev. Lett. 111, 027205 (2013)\nWang, X.S., Yan, P., Shen, Y.H., Bauer, G.E.W., Wang, X.R.: Domain wall propagation through spin wave emission. Phys. Rev. Lett. 109, 167209 (2012)",{"EN":1239},"Efficient manipulation of magnetic textures by spin–orbit torque is of great significance to spintronic and magnonic technologies. Here, using micromagnetic simulations, we exploit the dynamics of a Bloch-type stripe domain wall in a magnetic nanowire induced by the spin-Hall effect associated with a ferromagnet\u002Fheavy metal structure. Our numerical results demonstrate that, contrary to the Néel-type stripe domain wall, the stripe Bloch domain wall varies its internal spin configuration in response to the applied electric current and, in the meantime, travels toward an edge of the nanowire. The higher the current density applied, the nearer the domain wall approaches the edge. Thereby, the stripe Bloch domain wall is movable to any desired position with respect to the edge by fine-tuning the current density and\u002For its action time. These discoveries will find application in reconfigurable spin-wave channeling based on magnetic domain walls.",{"EN":1241},"Tailoring Bloch-type Stripe Domain Wall by Spin–orbit Torque for Reconfigurable Magnonic Waveguides",{"VOID":1243},"10.1007\u002Fs10948-022-06385-4","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs10948-022-06385-4",[1246,1272],{"id":1247,"sortIndex":181,"researcher":20,"roles":1248,"affiliations":1249,"properties":1269},"eaa4fc0d-9ce6-4352-969f-d5ac227dad8a",[241],[1250,1261],{"id":1251,"sortIndex":181,"affiliation":1252,"properties":1260},"92dea5fc-0f51-45ad-808c-c55c61c34efa",{"id":1253,"createTime":1254,"updateTime":1254,"relativeEntities":1255,"slug":1256,"properties":1257,"entityType":49,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"syncStatus":19,"languages":20,"translateLanguages":20,"viewCount":21},"1466f27b-6d25-46a0-b03e-0c461af685f1","2024-04-19T14:04:36.847+00:00",[],"Guangdong-Provincial-Key-Laboratory-of-Information-Photonics-Technology-Guangdong-University-of-Technology-Guangzhou-China",{"title":1258},{"EN":1259},"Guangdong Provincial Key Laboratory of Information Photonics Technology, Guangdong University of Technology, Guangzhou, 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