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Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals

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dc.contributor.author Srinivasu, V V
dc.date.accessioned 2010-08-25T13:43:56Z
dc.date.available 2010-08-25T13:43:56Z
dc.date.issued 2010-04
dc.identifier.citation Srinivasu, V V. 2010. Second and third peaks in the non-resonant microwave absorption spectra of superconducting bi2212 crystals. Journal of Superconductivity and novel magnetism, Vol. 23(3), pp 305-308 en
dc.identifier.issn 1557-1939
dc.identifier.uri http://www.springerlink.com/content/x446h30rg842q635/fulltext.pdf
dc.identifier.uri http://hdl.handle.net/10204/4211
dc.description Copyright: 2009 Springer Science and Business Media. This is the post print version. The definitive version is published in the Journal Journal of Superconductivity and Novel Magnetism, Vol. 23(3), pp 305-308 en
dc.description.abstract Non-resonant microwave absorption (NMA) measurements at liquid nitrogen temperature with systematic microwave power variation showed a two-peak structure in the Bi-2212 textured crystals, similar to that observed in the Bi-2212 single crystals (Srinivasu, et al., in J. Supercond. Incorp. Nov. Magn. 14:41, 2001). NMA signals from the aged Bi-2212 single crystals show an emergence of a ‘third peak’ as a function of microwave power. The authors qualitatively interpret these second and third peaks as due to the microwave power induced phase locking of several number of junctions into coherent groups and then the destruction of the phase locking by the applied DC field leading to decoupling or fluxon motion, which gives the loss in individual junctions belonging to these otherwise coherent groups. en
dc.language.iso en en
dc.publisher Springer Science and Business Media en
dc.subject Non-resonant microwave absorption en
dc.subject NMA en
dc.subject Fluxon motion en
dc.subject Bi2212 en
dc.subject Microwave en
dc.subject Superconductivity en
dc.subject Novel magnetism en
dc.title Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals en
dc.type Article en
dc.identifier.apacitation Srinivasu, V. V. (2010). Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals. http://hdl.handle.net/10204/4211 en_ZA
dc.identifier.chicagocitation Srinivasu, V V "Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals." (2010) http://hdl.handle.net/10204/4211 en_ZA
dc.identifier.vancouvercitation Srinivasu VV. Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals. 2010; http://hdl.handle.net/10204/4211. en_ZA
dc.identifier.ris TY - Article AU - Srinivasu, V V AB - Non-resonant microwave absorption (NMA) measurements at liquid nitrogen temperature with systematic microwave power variation showed a two-peak structure in the Bi-2212 textured crystals, similar to that observed in the Bi-2212 single crystals (Srinivasu, et al., in J. Supercond. Incorp. Nov. Magn. 14:41, 2001). NMA signals from the aged Bi-2212 single crystals show an emergence of a ‘third peak’ as a function of microwave power. The authors qualitatively interpret these second and third peaks as due to the microwave power induced phase locking of several number of junctions into coherent groups and then the destruction of the phase locking by the applied DC field leading to decoupling or fluxon motion, which gives the loss in individual junctions belonging to these otherwise coherent groups. DA - 2010-04 DB - ResearchSpace DP - CSIR KW - Non-resonant microwave absorption KW - NMA KW - Fluxon motion KW - Bi2212 KW - Microwave KW - Superconductivity KW - Novel magnetism LK - https://researchspace.csir.co.za PY - 2010 SM - 1557-1939 T1 - Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals TI - Second and third peaks in the non-resonant microwave absorption spectra of superconducting Bi2212 crystals UR - http://hdl.handle.net/10204/4211 ER - en_ZA


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