001     56561
005     20240708133730.0
024 7 _ |2 DOI
|a 10.1007/s10948-006-0124-4
024 7 _ |2 WOS
|a WOS:000244455700012
037 _ _ |a PreJuSER-56561
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Applied
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Jin, B. B.
|b 0
|u FZJ
|0 P:(DE-Juel1)VDB5630
245 _ _ |a Microwave and Terahertz Surface Resistance of MgB2 Thin Films
260 _ _ |a New York, NY
|b Springer
|c 2006
300 _ _ |a
336 7 _ |a Journal Article
|0 PUB:(DE-HGF)16
|2 PUB:(DE-HGF)
336 7 _ |a Output Types/Journal article
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336 7 _ |a Journal Article
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|2 EndNote
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a article
|2 DRIVER
440 _ 0 |a Journal of Superconductivity and Novel Magnetism
|x 1557-1939
|0 17001
|y 7
|v 19
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a The knowledge of the surface resistance R-s of superconducting thin film at microwave and terahertz (THz) regions is significant to design, make and assess superconducting microwave and THz electronic devices. In this paper we reported the R-s of MgB2 films at microwave and THz measured with sapphire resonator technique and the time-domain THz spectroscopy, respectively. Some interesting results are revealed in the following: ( 1) A clear correlation is found between R-s and normal-state resistivity right above T-c, p(0), i.e., R-s decreases almost linearly with the decrease of p(0). (2) A low residual R-s, less than 50 mu Omega at 18 GHz is achieved by different deposition techniques. In addition, between 10 and 14 K, MgB2 has the lowest Rs compared with two other superconductors Nb3Sn and the high-temperature superconductor YBa2Cu3O7-delta (YBCO). (3) From THz measurement it is found that the R-s of MgB2 up to around 1 THz is lower than that of copper and YBCO at the temperature below 25 K. (4) The frequency dependence of R-s follows omega(n), where omega is angular frequency, and n is power index. However, n changes from 1.9 at microwave to 1.5 at THz. The above results clearly give the evidences that MgB2 thin film, compared with other superconductors, is of advantage to make superconducting circuits working in the microwave and THz regions.
536 _ _ |a Erneuerbare Energien
|c P11
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|0 G:(DE-Juel1)FUEK401
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588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
|2 WoSType
700 1 _ |a Dahm, T.
|b 1
|0 P:(DE-HGF)0
700 1 _ |a Kadlec, F.
|b 2
|0 P:(DE-HGF)0
700 1 _ |a Kuzel, P.
|b 3
|0 P:(DE-HGF)0
700 1 _ |a Gubin, A. I.
|b 4
|u FZJ
|0 P:(DE-Juel1)VDB22375
700 1 _ |a Choi, E. M.
|b 5
|0 P:(DE-HGF)0
700 1 _ |a Kim, H. J.
|b 6
|0 P:(DE-HGF)0
700 1 _ |a Lee, S. I.
|b 7
|0 P:(DE-HGF)0
700 1 _ |a Kang, W. N.
|b 8
|0 P:(DE-HGF)0
700 1 _ |a Wang, S. F.
|b 9
|0 P:(DE-HGF)0
700 1 _ |a Zhou, Y. L.
|b 10
|0 P:(DE-HGF)0
700 1 _ |a Pogrebnyakov, A. V.
|b 11
|0 P:(DE-HGF)0
700 1 _ |a Redwing, J. M.
|b 12
|0 P:(DE-HGF)0
700 1 _ |a Xi, X. X.
|b 13
|0 P:(DE-HGF)0
700 1 _ |a Klein, N.
|b 14
|u FZJ
|0 P:(DE-Juel1)VDB5428
773 _ _ |a 10.1007/s10948-006-0124-4
|g Vol. 19
|q 19
|0 PERI:(DE-600)2246896-1
|t Journal of superconductivity and novel magnetism
|v 19
|y 2006
|x 1557-1939
909 C O |o oai:juser.fz-juelich.de:56561
|p VDB
913 1 _ |k P11
|v Erneuerbare Energien
|l Erneuerbare Energien
|b Energie
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914 1 _ |a Nachtrag
|y 2006
915 _ _ |0 StatID:(DE-HGF)0010
|a JCR/ISI refereed
920 1 _ |k IPV
|l Institut für Photovoltaik
|d 31.12.2006
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|0 I:(DE-Juel1)VDB46
|x 1
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