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Ovcharenko, and Yu. F. Smirnov, Microscopic Theory of Collective Excitations in Nuclei (Nauk. Dumka, Kiev, 1981).",{},{"id":18,"text":447,"url":18,"identifiers":448},"Yu. F. Smirnov et al., Nucl. Phys. A 235, 289 (1974).",{"doi":449},"10.1016\u002F0375-9474(74)90193-6",{"id":18,"text":451,"url":18,"identifiers":452},"R. B. Firestone and V. S. Shirley, Table of Isotropes (Wiley, New York, 1996).",{},{"id":18,"text":454,"url":18,"identifiers":455},"M. Freer et al., Phys. Rev. Lett. 96, 042501 (2006).",{"doi":456},"10.1103\u002FPhysRevLett.96.042501",{"id":18,"text":458,"url":18,"identifiers":459},"R. Volski, I. A. Gnilozub, S. D. Kurgalin, A. V. Sinyakov, and Yu. M. Tchuvil’sky, Izv. Akad. Nauk, Ser. Fiz. 72, 1291 (2008).",{},{"id":18,"text":461,"url":18,"identifiers":462},"V. Z. Gol’dberg, V. I. Dukhanov, A. E. Pakhomov, et al., Yad. Fiz. 60, 1186 (1997) [Phys. At. Nucl. 60, 1061 (1997)].",{},{"id":18,"text":464,"url":18,"identifiers":465},"M. Freer et al., Phys. Rev. Lett. 82, 1383 (1999).",{"doi":466},"10.1103\u002FPhysRevLett.82.1383",{"id":18,"text":468,"url":18,"identifiers":469},"H. G. Bohlen et al., Nucl. Phys. A 722, 3c (2003).",{"doi":470},"10.1016\u002FS0375-9474(03)01327-7",{"id":472,"createTime":473,"updateTime":474,"relativeEntities":475,"slug":476,"properties":477,"entityType":189,"verifyStatus":190,"verifyTime":488,"verifyNote":192,"languages":18,"translateLanguages":18,"viewCount":19,"primaryUrl":489,"fullTextUrl":18,"authors":490,"publicationType":227,"publisherRelationship":531,"citationCount":18,"citationInfo":18,"publishDate":582,"publishYear":583,"citationAnalyzeStatus":584,"lastCitationAnalyze":585,"indexDatabases":586,"openAccess":18,"references":18,"isForceReanalyzing":277},"5f353f7c-1f98-4b4a-8103-fc9503dbb9a7","2024-02-06T17:27:59.872+00:00","2026-08-18T12:38:54.785+00:00",[],"Neutrino-masses-nuclear-matrix-elements-and-the-0%CE%BD%CE%B2%CE%B2-decay-of-76Ge",{"abstract":478,"title":480,"gsPaper":482,"references":484,"doi":486},{"EN":479},"Neutrino data, obtained from SNO, SK, CHOOZ, KamLAND, and WMAP, are used to establish the upper limit of 〈m\nν〉 relevant for the 0νββ. The decay of 76Ge is discussed within different light-neutrino mass spectra and with different nuclear matrix elements.",{"EN":481},"Neutrino masses, nuclear matrix elements, and the 0νββ decay of 76Ge",{"VOID":483},"[\"6885179680098746320\"]",{"VOID":485},"Q. R. Ahmad et al. (SNO Collab.), Phys. Rev. Lett. 87, 071301 (2001); 89, 011301 (2002); 89, 011302 (2002).\nS. Fukuda et al. (Super-Kamiokande Collab.), Phys. Rev. Lett. 86, 5651 (2001).\nK. Eguchi et al. (KamLAND Collab.), Phys. Rev. Lett. 90, 021802 (2003).\nM. Appollonio et al., Phys. Lett. B 466, 415 (1999).\nC. L. Bennet et al., astro-ph\u002F0302207.\nS. Pascoli, S. T. Petcov, and W. Rodejohann, hep-ph\u002F0209059; hep-ph\u002F0212113.\nL. Wolfenstein, Phys. Rev. D 17, 2369 (1978); S. P. Mikheev and A. Y. Smirnov, Yad. Fiz. 42, 1441 (1985) [Sov. J. Nucl. Phys. 42, 913 (1985)].\nA. Y. Smirnov, Czech. J. Phys. 52, 439 (2002).\nH. V. Klapdor-Kleingrothhaus, H. Päs, and A. Y. Smirnov, Phys. Rev. D 63, 073005 (2001).\nE. Ma, hep-ph\u002F0303126.\nH. V. Klapdor-Kleingrothaus, A. Dietz, H. L. Harney, and I. V. Krivosheina, Mod. Phys. Lett. A 16, 2409 (2001); H. V. Klapdor-Kleingrothaus et al., Part. Nucl. Lett. 110 (1), 57 (2002).\nC. E. Aalseth et al., hep-ex\u002F0202018; Mod. Phys. Lett. A 17, 1475 (2002).\nA. Bandyopadhyay, S. Choubey, S. Goswami, and K. Kar, hep-ph\u002F0110307; Phys. Rev. D 65, 073031 (2002).\nJ. Suhonen and O. Civitarese, Phys. 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A 629, 605 (1998).\nR. Anne et al., Nucl. Instrum. Methods Phys. Res. A 257, 215 (1987).\nR. Anne, Preprint GANIL, GANIL P02 01 (2000).\nP. Moller et al., At. Data Nucl. Data Tables 39, 225 (1988).\nG. A. Lalazissis et al., Phys. Rev. C 60, 014310 (1999).\nE. Caurier et al., Phys. Rev. C 58, 2033 (1998).\nY. Utsuno et al., Phys. Rev. C 64, 011301 (2001).\nZ. Ren et al., Phys. Rev. C 52, R20 (1995).\nJ. Terasaki et al., Nucl. Phys. 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Phys. 44, 291 (1970).",{"VOID":1175},"10.1134\u002FS1063778808020178","2024-06-25T02:44:04.769+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1134\u002FS1063778808020178",[1179,1194],{"id":1180,"sortIndex":19,"researcher":18,"roles":1181,"affiliations":1182,"properties":1191,"displayName":1193,"givenName":18,"familyName":18},"bec7465d-2e3e-41a9-9f90-a5985b9298f7",[200],[1183],{"id":1184,"sortIndex":19,"affiliation":1185,"properties":18},"17614579-7e28-4efb-b9fb-c1dfa39d8eba",{"id":1184,"createTime":18,"updateTime":18,"relativeEntities":1186,"slug":18,"properties":1187,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1190,"statistic":18},[],{"title":1188},{"VI":1189},"Institute of Theoretical and Experimental Physics, Moscow, Russia",[],{"title":1192},{"VI":1193},"B. O. Kerbikov",{"id":1195,"sortIndex":215,"researcher":18,"roles":1196,"affiliations":1197,"properties":1204,"displayName":1206,"givenName":18,"familyName":18},"5b6ad474-ee18-46ee-ab36-c5d004d016ee",[200],[1198],{"id":1184,"sortIndex":19,"affiliation":1199,"properties":18},{"id":1184,"createTime":18,"updateTime":18,"relativeEntities":1200,"slug":18,"properties":1201,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1203,"statistic":18},[],{"title":1202},{"VI":1189},[],{"title":1205},{"VI":1206},"E. V. Luschevskaya",{"url":1177,"publisher":1208,"properties":1253},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1209,"slug":10,"properties":1210,"entityType":16,"verifyStatus":17,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":19,"subjectFields":1213,"manageAffiliations":1222,"indexDatabases":1233,"url":18,"thumbnailPath":18,"statistic":1248,"gsStatistic":18,"type":166,"analyzePriority":18},[],{"issn":1211,"title":1212},{"VOID":13},{"VOID":15},[1214,1218],{"id":22,"createTime":18,"updateTime":18,"relativeEntities":1215,"label":1216,"description":1217,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":25},{},{"id":28,"createTime":18,"updateTime":18,"relativeEntities":1219,"label":1220,"description":1221,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":31},{},[1223,1228],{"id":35,"createTime":18,"updateTime":18,"relativeEntities":1224,"slug":18,"properties":1225,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1227,"statistic":18},[],{"title":1226},{"EN":39},[],{"id":42,"createTime":18,"updateTime":18,"relativeEntities":1229,"slug":18,"properties":1230,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1232,"statistic":18},[],{"title":1231},{"EN":46},[],[1234,1241],{"id":67,"indexDatabase":1235,"url":78,"indexYears":79,"academicFieldIds":1240,"indexDatabaseRanking":83},{"id":69,"createTime":18,"updateTime":18,"relativeEntities":1236,"label":1237,"description":1238,"key":75,"publicationTags":1239,"standard":18},[],{"EN":72,"VI":72},{"EN":72,"VI":74},[77],[81,82],{"id":50,"indexDatabase":1242,"url":63,"indexYears":18,"academicFieldIds":1247,"indexDatabaseRanking":18},{"id":52,"createTime":18,"updateTime":18,"relativeEntities":1243,"label":1244,"description":1245,"key":59,"publicationTags":1246,"standard":18},[],{"EN":55,"VI":55},{"EN":57,"VI":58},[61,62],[65],{"impactFactor":19,"impactFactorByYear":1249,"i10Index":95,"i10IndexLast5Year":96,"totalPublication":97,"totalPublicationByYear":1250,"totalCitation":121,"totalCitationByYear":1251,"totalCitationPerPublication":144,"totalCitationPerPublicationByYear":1252,"hindexLast5Year":142,"hindex":142},{"2010":86,"2011":19,"2012":87,"2013":88,"2014":89,"2015":90,"2016":88,"2017":91,"2018":88,"2019":92,"2020":93,"2021":90,"2022":89,"2023":94},{"2000":99,"2001":100,"2002":101,"2003":102,"2004":103,"2005":104,"2006":105,"2007":106,"2008":107,"2009":101,"2010":108,"2011":109,"2012":105,"2013":110,"2014":111,"2015":112,"2016":113,"2017":114,"2018":115,"2019":116,"2020":117,"2021":118,"2022":110,"2023":119,"2024":120},{"2000":123,"2001":124,"2002":125,"2003":126,"2004":110,"2005":127,"2006":128,"2007":129,"2008":105,"2009":130,"2010":131,"2011":132,"2012":112,"2013":133,"2014":134,"2015":135,"2016":136,"2017":137,"2018":138,"2019":139,"2020":140,"2021":141,"2022":142,"2023":143},{"2000":146,"2001":147,"2002":148,"2003":149,"2004":150,"2005":151,"2006":152,"2007":153,"2008":154,"2009":155,"2010":156,"2011":157,"2012":158,"2013":155,"2014":155,"2015":159,"2016":160,"2017":161,"2018":162,"2019":158,"2020":163,"2021":164,"2022":164,"2023":165},{"pages":1254,"volume":1256},{"VOID":1255},"364-373",{"VOID":1257},"71",{"total":19,"publishYear":1259,"statisticByYear":1260},2011,{},"2011-03-11",[83,61],{"id":1264,"createTime":1265,"updateTime":1266,"relativeEntities":1267,"slug":1268,"properties":1269,"entityType":189,"verifyStatus":190,"verifyTime":1280,"verifyNote":192,"languages":18,"translateLanguages":18,"viewCount":19,"primaryUrl":1281,"fullTextUrl":18,"authors":1282,"publicationType":227,"publisherRelationship":1375,"citationCount":19,"citationInfo":1425,"publishDate":1427,"publishYear":583,"citationAnalyzeStatus":584,"lastCitationAnalyze":1428,"indexDatabases":1429,"openAccess":18,"references":18,"isForceReanalyzing":277},"9e41e0ee-ed3e-4187-813a-7c6c9827c3b6","2024-01-20T03:15:57.280+00:00","2026-07-28T18:22:31.683+00:00",[],"Features-of-pC-interactions-at-a-momentum-of-4-2-GeV-c-versus-the-degree-of-centrality-of-a-collision-between-a-proton-and-a-carbon-nucleus-Kinematical-features-of-secondaries",{"abstract":1270,"title":1272,"gsPaper":1274,"references":1276,"doi":1278},{"EN":1271},"The mean values of the momenta and emission angles of charged pions and protons in the laboratory frame are presented both for the total ensemble of interactions between 4.2-GeV\u002Fc protons and a carbon nucleus and for six groups of events characterized by different degrees of collision centrality. The distributions with respect to the total and the transverse momentum are presented for the particles being studied, along with the longitudinal-rapidity distributions. Our experimental data are compared with the predictions of the cascade-evaporation model and of two versions of the refined FRITIOF model. It is shown that, as the degree of collision centrality becomes higher, the mean momenta and rapidities of secondaries decrease, the transverse momenta remain virtually unchanged, and the mean angles of particle emission increase. This is consistent with the pattern of particle cascading in nuclei. However, the mean transverse momentum 〈p\n\n                  t\n                〉 of participant protons that was obtained on the basis of the cascade-evaporation model decreases with increasing degree of collision centrality, in contrast to what is observed in our experiment. A satisfactory description of experimental data is on the basis of the refined FRITIOF model taking into account Δ+ and Δ0 isobars. The stopping power of carbon nuclei for 4.2-GeV\u002Fc protons is also determined.",{"EN":1273},"Features of pC interactions at a momentum of 4.2 GeV\u002Fc versus the degree of centrality of a collision between a proton and a carbon nucleus: Kinematical features of secondaries",{"VOID":1275},"[\"13921938072546012996\"]",{"VOID":1277},"G. N. Agakishiev et al., Yad. Fiz. 40, 1209 (1984) [Sov. J. Nucl. Phys. 39, 344 (1984)]; G. N. Agakishiev et al., Z. Phys. C 27, 177 (1985).\nG. N. Agakishiev et al., Yad. Fiz. 45, 1047 (1987) [Sov. J. Nucl. Phys. 45, 1037 (1987)]; D. Armutliisky et al., Z. Phys. A 328, 455 (1987).\nG. N. Agakishiev et al., Yad. Fiz. 49, 481 (1989) [Sov. J. Nucl. Phys. 49, 300 (1989)].\nA. I. Bondarenko, R. A. Bondarenko, and E. N. Kladnitskaya, Yad. Fiz. 60, 2004 (1997) [Phys. At. Nucl. 60, 1833 (1997)].\nA. I. Bondarenko et al., Yad. 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OIYaI No. R1-98-292 (Dubna, 1998).",{"VOID":1279},"10.1134\u002F1.1648916","2024-08-31T01:15:40.314+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1134\u002F1.1648916",[1283,1305,1318,1340,1362],{"id":1284,"sortIndex":19,"researcher":18,"roles":1285,"affiliations":1286,"properties":1302,"displayName":1304,"givenName":18,"familyName":18},"6d7931d3-0300-496e-a3d0-429e3d222675",[200],[1287,1295],{"id":1288,"sortIndex":19,"affiliation":1289,"properties":18},"79e1f810-bd73-41a6-814b-c74a85d533aa",{"id":1288,"createTime":18,"updateTime":18,"relativeEntities":1290,"slug":18,"properties":1291,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1294,"statistic":18},[],{"title":1292},{"VI":1293},"Yerevan Physics Institute, Yerevan, Armenia",[],{"id":611,"sortIndex":215,"affiliation":1296,"properties":1301},{"id":611,"createTime":18,"updateTime":18,"relativeEntities":1297,"slug":18,"properties":1298,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1300,"statistic":18},[],{"title":1299},{"VI":616},[],{},{"title":1303},{"VI":1304},"A. 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For this effect to emerge, it is necessary that the vector current not be conserved; in the ξ gauge, there arise additional complications because of the presence of an unphysical scalar field. Solutions to the Dyson-Schwinger equations are obtained, and the renormalization of complete propagators is investigated. The use of the Ward identity, which relates a few different Green's functions, is a key point in performing this renormalization. It is shown that the dependence on the gauge parameter ξ disappears in the renormalized matrix element.",{"EN":1440},"Unitary scalar-vector mixing in the ξ gauge",{"VOID":1442},"[\"555097670357320541\"]",{"VOID":1444},"L. Baulieu and R. Coquereaux, Ann. Phys. (N.Y.) 140, 163 (1982).\nK. Aoki et al., Prog. Theor. Phys. Suppl. 73, 1 (1982).\nA. E. Kaloshin, Yad. Fiz. 60, 1306 (1997) [Phys. At. Nucl. 60, 1179 (1997)].\nM. C. Peyranere, Int. J. Mod. Phys. A 14, 429 (1999).\nHung Cheng and S. P. Li, hep-ph\u002F0107103.\nJ. C. Taylor, Gauge Theories of Weak Interaction (Cambridge Univ. Press, Cambridge, 1976; Mir, Moscow, 1978).\nS. Gasiorowicz and D. A. Geffen, Rev. Mod. Phys. 41, 531 (1969).\nM. K. Volkov, Fiz. Élem. Chastits At. Yadra 17, 433 (1986) [Sov. J. Part. Nucl. 17, 186 (1986)].\nN. N. Bogolyubov and D. V. Shirkov, Introduction to the Theory of Quantized Fields (Nauka, Moscow, 1976).\nG. Passarino, Nucl. Phys. B 574, 451 (2000).",{"VOID":1446},"10.1134\u002F1.1592592","2024-06-25T14:51:31.091+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1134\u002F1.1592592",[1450,1465],{"id":1451,"sortIndex":19,"researcher":18,"roles":1452,"affiliations":1453,"properties":1462,"displayName":1464,"givenName":18,"familyName":18},"51deb9ef-8f86-4236-bbff-2da88fe65050",[200],[1454],{"id":1455,"sortIndex":19,"affiliation":1456,"properties":18},"6d388407-9ba7-460f-82d8-698c77d2534b",{"id":1455,"createTime":18,"updateTime":18,"relativeEntities":1457,"slug":18,"properties":1458,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1461,"statistic":18},[],{"title":1459},{"VI":1460},"Institute of Applied Physics, Irkutsk State University, Irkutsk, Russia",[],{"title":1463},{"VI":1464},"A. E. 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It is shown that the temperature of the phase transition decreases in relation to the case of zero magnetic field.",{"EN":1543},"Temperature deconfinement in QCD in a magnetic field",{"VOID":1545},"[\"17709685234061357080\"]",{"VOID":1547},"S. Weinberg, Physica A 96, 327 (1979).\nJ. Gasser and H. Leutwyler, Ann. Phys. (N.Y.) 158, 142 (1984).\nJ. Gasser and H. Leutwyler, Nucl. Phys. B 250, 465 (1985).\nP. Binétrui and M. K. Gaillard, Phys. Rev. D 32, 931 (1985).\nJ. Gasser and H. Leutwyler, Phys. Lett. B 184, 83 (1987).\nJ. Gasser and H. Leutwyler, Phys. Lett. B 188, 477 (1987).\nH. Neuberger, Phys. Rev. Lett. 60, 889 (1988).\nH. Leutwyler, Nucl. Phys. B (Proc. Suppl.) 4, 248 (1988).\nP. Gerber and H. Leutwyler, Nucl. Phys. B 321, 387 (1989).\nN. O. Agasian, Phys. Lett. B 519, 71 (2001); JETP Lett. 74, 353 (2001).\nS. P. Klevansky and R. H. Lemmer, Phys. Rev. D 39, 3478 (1989).\nI. A. Shushpanov and A. V. Smilga, Phys. Lett. B 402, 351 (1997).\nN. O. Agasian and I. A. Shushpanov, JETP Lett. 70, 717 (1999); Phys. Lett. B 472, 143 (2000).\nN. O. Agasian, Phys. Lett. B 488, 39 (2000); Yad Fiz. 64, 608, 2001; Phys. At. Nucl. 64, 554 (2001).\nD. Ebert, V. C. Zhukovsky, and A. S. Vshivtsev, Int. J.Mod. Phys. A 13, 1723 (1998).\nN. O. Agasian, B. O. Kerbikov, and V. I. Shevchenko, Phys. Rep. 320, 131 (1999).\nV. Skalozub and M. Bordag, Nucl. Phys. B 576, 430 (2000).\nV.V. Skalozub and A. V. Strelchenko, Eur. Phys. J.C 33, 105 (2004).\nP. Cea and L. Cosmai, J. High Energy Phys. 0302, 031 (2003).\nN. O. Agasian, Pis’ma Zh. Éksp. Teor. Fiz. 71, 65 (2000) [JETP Lett. 71, 43 (2000)].\nN. O. Agasian and K. Zarembo, Phys. Rev. D 57, 2475 (1998).\nN. O. Agasian and I. A. Shushpanov, J. High Energy Phys. 0110, 006 (2001).\nD. Kabat, K. M. Lee, and E. Weinberg, Phys. Rev. D 66, 014004 (2002).\nV. A. Miransky and I. A. Shovkovy, Phys. Rev. D 66, 045006 (2002).\nT. D. Cohen, D. A. McGady, and E. S. Werbos, Phys. Rev. C 76, 055201 (2007).\nB. O. Kerbikov and E. V. Lushevskaya, Yad. Fiz. 71, 385 (2008) [Phys. At. Nucl. 71, 364 (2008)].\nYu. A. Simonov, Pis’ma Zh. Éksp. Teor. Fiz. 55, 605 (1992) [JETP Lett. 55, 627 (1992)].\nN. O. Agasian, Pis’ma Zh. Éksp. Teor. Fiz. 57, 200 (1993) [JETP Lett. 57, 208 (1993)]; Phys. Lett. B 562, 257 (2003).\nM. D’Elia, A. Di Giacomo, and E. Meggiolaro, Phys. Rev. D 67, 114504 (2003).",{"VOID":1549},"10.1134\u002FS1063778809020215","2024-07-11T01:35:30.306+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1134\u002FS1063778809020215",[1553],{"id":1554,"sortIndex":19,"researcher":18,"roles":1555,"affiliations":1556,"properties":1563,"displayName":1565,"givenName":18,"familyName":18},"8e83bf80-2a01-4a95-8f68-b8d783d8e926",[200],[1557],{"id":1184,"sortIndex":19,"affiliation":1558,"properties":18},{"id":1184,"createTime":18,"updateTime":18,"relativeEntities":1559,"slug":18,"properties":1560,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1562,"statistic":18},[],{"title":1561},{"VI":1189},[],{"title":1564},{"VI":1565},"N. O. Agasian",{"url":1551,"publisher":1567,"properties":1612},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1568,"slug":10,"properties":1569,"entityType":16,"verifyStatus":17,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":19,"subjectFields":1572,"manageAffiliations":1581,"indexDatabases":1592,"url":18,"thumbnailPath":18,"statistic":1607,"gsStatistic":18,"type":166,"analyzePriority":18},[],{"issn":1570,"title":1571},{"VOID":13},{"VOID":15},[1573,1577],{"id":22,"createTime":18,"updateTime":18,"relativeEntities":1574,"label":1575,"description":1576,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":25},{},{"id":28,"createTime":18,"updateTime":18,"relativeEntities":1578,"label":1579,"description":1580,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":31},{},[1582,1587],{"id":35,"createTime":18,"updateTime":18,"relativeEntities":1583,"slug":18,"properties":1584,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1586,"statistic":18},[],{"title":1585},{"EN":39},[],{"id":42,"createTime":18,"updateTime":18,"relativeEntities":1588,"slug":18,"properties":1589,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1591,"statistic":18},[],{"title":1590},{"EN":46},[],[1593,1600],{"id":67,"indexDatabase":1594,"url":78,"indexYears":79,"academicFieldIds":1599,"indexDatabaseRanking":83},{"id":69,"createTime":18,"updateTime":18,"relativeEntities":1595,"label":1596,"description":1597,"key":75,"publicationTags":1598,"standard":18},[],{"EN":72,"VI":72},{"EN":72,"VI":74},[77],[81,82],{"id":50,"indexDatabase":1601,"url":63,"indexYears":18,"academicFieldIds":1606,"indexDatabaseRanking":18},{"id":52,"createTime":18,"updateTime":18,"relativeEntities":1602,"label":1603,"description":1604,"key":59,"publicationTags":1605,"standard":18},[],{"EN":55,"VI":55},{"EN":57,"VI":58},[61,62],[65],{"impactFactor":19,"impactFactorByYear":1608,"i10Index":95,"i10IndexLast5Year":96,"totalPublication":97,"totalPublicationByYear":1609,"totalCitation":121,"totalCitationByYear":1610,"totalCitationPerPublication":144,"totalCitationPerPublicationByYear":1611,"hindexLast5Year":142,"hindex":142},{"2010":86,"2011":19,"2012":87,"2013":88,"2014":89,"2015":90,"2016":88,"2017":91,"2018":88,"2019":92,"2020":93,"2021":90,"2022":89,"2023":94},{"2000":99,"2001":100,"2002":101,"2003":102,"2004":103,"2005":104,"2006":105,"2007":106,"2008":107,"2009":101,"2010":108,"2011":109,"2012":105,"2013":110,"2014":111,"2015":112,"2016":113,"2017":114,"2018":115,"2019":116,"2020":117,"2021":118,"2022":110,"2023":119,"2024":120},{"2000":123,"2001":124,"2002":125,"2003":126,"2004":110,"2005":127,"2006":128,"2007":129,"2008":105,"2009":130,"2010":131,"2011":132,"2012":112,"2013":133,"2014":134,"2015":135,"2016":136,"2017":137,"2018":138,"2019":139,"2020":140,"2021":141,"2022":142,"2023":143},{"2000":146,"2001":147,"2002":148,"2003":149,"2004":150,"2005":151,"2006":152,"2007":153,"2008":154,"2009":155,"2010":156,"2011":157,"2012":158,"2013":155,"2014":155,"2015":159,"2016":160,"2017":161,"2018":162,"2019":158,"2020":163,"2021":164,"2022":164,"2023":165},{"pages":1613,"volume":1615},{"VOID":1614},"339-342",{"VOID":1616},"72",{"total":19,"publishYear":1618,"statisticByYear":1619},2009,{},"2009-02-25","2026-07-25T22:58:07.217+00:00",[83,61],{"id":1624,"createTime":1625,"updateTime":1626,"relativeEntities":1627,"slug":1628,"properties":1629,"entityType":189,"verifyStatus":190,"verifyTime":1640,"verifyNote":192,"languages":18,"translateLanguages":18,"viewCount":19,"primaryUrl":1641,"fullTextUrl":18,"authors":1642,"publicationType":227,"publisherRelationship":1690,"citationCount":19,"citationInfo":1741,"publishDate":1744,"publishYear":1742,"citationAnalyzeStatus":584,"lastCitationAnalyze":1745,"indexDatabases":1746,"openAccess":18,"references":18,"isForceReanalyzing":277},"dbfb6b33-1180-4d87-8140-4964d8d08430","2024-01-24T22:59:36.648+00:00","2026-07-24T13:47:54.416+00:00",[],"Self-Consistent-Calculation-of-the-Charge-Radii-in-a-Long-mathbf-58-82-Cu-Isotopic-Chain",{"abstract":1630,"title":1632,"gsPaper":1634,"references":1636,"doi":1638},{"EN":1631},"The charge radii are calculated in long chain of copper isotopes that includes the \n                  \n                    \n                  \n                  $${}^{58,79}$$\n                  \n                Cu exotic nuclei, which are close to the doubly magic nuclei of \n                  \n                    \n                  \n                  $${}^{58,78}$$\n                  \n                Ni, and the nuclei featuring the \n                  \n                    \n                  \n                  $$N=32$$\n                  \n                , \n                  \n                    \n                  \n                  $$34$$\n                  \n                , and \n                  \n                    \n                  \n                  $$40$$\n                  \n                 magic subshells. Use is made of the self-consistent theory of finite Fermi systems and the family of energy density functionals proposed by Fayans and his coauthors (DF3, DF3-a, …). The results are compared with experimental data and with the results of the calculations based on self-consistent models that employ new versions of the Fayans functional—Fy(std) and Fy(HFB, \n                  \n                    \n                  \n                  $$\\nabla r$$\n                  \n                ), whose parameters were obtained by means of an extended optimization protocol—as well as with the results of ab-initio calculations performed on the basis of the renormalization-group model and with the results of the calculation with a density-dependent spin–orbit interaction stemming from three-nucleon forces. The weakening of odd–even staggering of radii of nuclei in the ISOLDE-CERN experiments as the nuclei approach the \n                  \n                    \n                  \n                  $$N=50$$\n                  \n                 closed neutron shell is analyzed, and the possible mechanisms behind this weakening are considered. It is shown that the isotopic dependences of the charge radii and the total beta-decay energies are correlated.",{"EN":1633},"Self-Consistent Calculation of the Charge Radii in a Long $${}^{\\mathbf{58{-}82}}$$ Cu Isotopic Chain",{"VOID":1635},"[\"13340113765460541900\"]",{"VOID":1637},"V. E. Fortov, B. Yu. Sharkov, and H. Stöker, Phys. Usp. 55, 582 (2012).\nExtreme Light Fields Research Center Project xcels, Inst. Appl. Phys., Russ. Acad. Sci. http:\u002F\u002Fwww.xcels.iapras.ru.\nI. Angeli and K. P. Marinova, At. Data Nucl. Data Tables 99, 69 (2013).\nT. E. Cocolios, H. H. Al Suradi, J. Billowes, I. Budinčević, R. P. de Groote, S. 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Usp. 63, 209 (2020). https:\u002F\u002Fdoi.org\u002F10.3367\u002FUFNe.2019.03.038547",{"VOID":1639},"10.1134\u002FS1063778820060101","2024-06-22T23:19:12.875+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1134\u002FS1063778820060101",[1643,1668],{"id":1644,"sortIndex":19,"researcher":18,"roles":1645,"affiliations":1646,"properties":1663,"displayName":1665,"givenName":18,"familyName":18},"7ebc4fab-d9b4-4266-8f47-4783e73f2961",[200],[1647,1655],{"id":1648,"sortIndex":19,"affiliation":1649,"properties":18},"0b0ee483-3852-48bc-b3d4-ecfa4390b033",{"id":1648,"createTime":18,"updateTime":18,"relativeEntities":1650,"slug":18,"properties":1651,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1654,"statistic":18},[],{"title":1652},{"VI":1653},"National Research Center Kurchatov Institute, Moscow, Russia",[],{"id":1656,"sortIndex":215,"affiliation":1657,"properties":18},"177b584f-71d9-4342-b86e-375b82fc7b6f",{"id":1656,"createTime":18,"updateTime":18,"relativeEntities":1658,"slug":18,"properties":1659,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1662,"statistic":18},[],{"title":1660},{"VI":1661},"Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna, Russia",[],{"title":1664,"gsAuthor":1666},{"VI":1665},"I. 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Borzov",{"VOID":1667},"[\"erV1GIQAAAAJ\"]",{"id":1669,"sortIndex":215,"researcher":18,"roles":1670,"affiliations":1671,"properties":1687,"displayName":1689,"givenName":18,"familyName":18},"3d55a6ea-a7ac-4ad1-b3e0-3a98f9b04fbf",[200],[1672,1678],{"id":1648,"sortIndex":19,"affiliation":1673,"properties":18},{"id":1648,"createTime":18,"updateTime":18,"relativeEntities":1674,"slug":18,"properties":1675,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1677,"statistic":18},[],{"title":1676},{"VI":1653},[],{"id":1679,"sortIndex":215,"affiliation":1680,"properties":1686},"5a71ece0-708f-4516-9697-b7911e0cee09",{"id":1679,"createTime":18,"updateTime":18,"relativeEntities":1681,"slug":18,"properties":1682,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1685,"statistic":18},[],{"title":1683},{"VI":1684},"Moscow Institute of Physics and Technology (State University), Dolgoprudnyi, Russia",[],{},{"title":1688},{"VI":1689},"S. 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Tolokonnikov",{"url":1641,"publisher":1691,"properties":1736},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1692,"slug":10,"properties":1693,"entityType":16,"verifyStatus":17,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":19,"subjectFields":1696,"manageAffiliations":1705,"indexDatabases":1716,"url":18,"thumbnailPath":18,"statistic":1731,"gsStatistic":18,"type":166,"analyzePriority":18},[],{"issn":1694,"title":1695},{"VOID":13},{"VOID":15},[1697,1701],{"id":22,"createTime":18,"updateTime":18,"relativeEntities":1698,"label":1699,"description":1700,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":25},{},{"id":28,"createTime":18,"updateTime":18,"relativeEntities":1702,"label":1703,"description":1704,"parentId":18,"standard":18,"scholarHubFieldId":18},[],{"EN":31},{},[1706,1711],{"id":35,"createTime":18,"updateTime":18,"relativeEntities":1707,"slug":18,"properties":1708,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1710,"statistic":18},[],{"title":1709},{"EN":39},[],{"id":42,"createTime":18,"updateTime":18,"relativeEntities":1712,"slug":18,"properties":1713,"entityType":18,"verifyStatus":18,"verifyTime":18,"verifyNote":18,"languages":18,"translateLanguages":18,"viewCount":18,"url":18,"parentIds":1715,"statistic":18},[],{"title":1714},{"EN":46},[],[1717,1724],{"id":67,"indexDatabase":1718,"url":78,"indexYears":79,"academicFieldIds":1723,"indexDatabaseRanking":83},{"id":69,"createTime":18,"updateTime":18,"relativeEntities":1719,"label":1720,"description":1721,"key":75,"publicationTags":1722,"standard":18},[],{"EN":72,"VI":72},{"EN":72,"VI":74},[77],[81,82],{"id":50,"indexDatabase":1725,"url":63,"indexYears":18,"academicFieldIds":1730,"indexDatabaseRanking":18},{"id":52,"createTime":18,"updateTime":18,"relativeEntities":1726,"label":1727,"description":1728,"key":59,"publicationTags":1729,"standard":18},[],{"EN":55,"VI":55},{"EN":57,"VI":58},[61,62],[65],{"impactFactor":19,"impactFactorByYear":1732,"i10Index":95,"i10IndexLast5Year":96,"totalPublication":97,"totalPublicationByYear":1733,"totalCitation":121,"totalCitationByYear":1734,"totalCitationPerPublication":144,"totalCitationPerPublicationByYear":1735,"hindexLast5Year":142,"hindex":142},{"2010":86,"2011":19,"2012":87,"2013":88,"2014":89,"2015":90,"2016":88,"2017":91,"2018":88,"2019":92,"2020":93,"2021":90,"2022":89,"2023":94},{"2000":99,"2001":100,"2002":101,"2003":102,"2004":103,"2005":104,"2006":105,"2007":106,"2008":107,"2009":101,"2010":108,"2011":109,"2012":105,"2013":110,"2014":111,"2015":112,"2016":113,"2017":114,"2018":115,"2019":116,"2020":117,"2021":118,"2022":110,"2023":119,"2024":120},{"2000":123,"2001":124,"2002":125,"2003":126,"2004":110,"2005":127,"2006":128,"2007":129,"2008":105,"2009":130,"2010":131,"2011":132,"2012":112,"2013":133,"2014":134,"2015":135,"2016":136,"2017":137,"2018":138,"2019":139,"2020":140,"2021":141,"2022":142,"2023":143},{"2000":146,"2001":147,"2002":148,"2003":149,"2004":150,"2005":151,"2006":152,"2007":153,"2008":154,"2009":155,"2010":156,"2011":157,"2012":158,"2013":155,"2014":155,"2015":159,"2016":160,"2017":161,"2018":162,"2019":158,"2020":163,"2021":164,"2022":164,"2023":165},{"pages":1737,"volume":1739},{"VOID":1738},"828-840",{"VOID":1740},"83",{"total":19,"publishYear":1742,"statisticByYear":1743},2021,{},"2021-02-11","2026-07-24T13:47:54.415+00:00",[83,61]]