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024 7 _ |a 10.1103/PhysRevB.81.054522
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041 _ _ |a eng
082 _ _ |a 530
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|a Physics, Condensed Matter
100 1 _ |0 P:(DE-HGF)0
|a Kemmler, M.
|b 0
245 _ _ |a Magnetic interference patterns in 0-pi superconductor/insulator/ferromagnet/superconductor Josephson junctions: Effects of asymmetry between 0 and pi regions
260 _ _ |a College Park, Md.
|b APS
|c 2010
300 _ _ |a 054522
336 7 _ |a Journal Article
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440 _ 0 |0 4919
|a Physical Review B
|v 81
|x 1098-0121
|y 5
500 _ _ |a This work is supported by the Deutsche Forschungsgemeinschaft (DFG) via the SFB/TRR 21 and Projects No. GO 944/3 and KO 1303/3. M. Kemmler acknowledges support by the Carl-Zeiss Stiftung. M. Weides is supported by DFG under Project No. WE 4359/1-1.
520 _ _ |a We present a detailed analysis of the dependence of the critical current I-c on an in-plane magnetic field B of 0, pi, and 0-pi superconductor-insulator-ferromagnet-superconductor Josephson junctions. I-c(B) of the 0 and the pi junction closely follows a Fraunhofer pattern, indicating a homogeneous critical current density j(c)(x). The maximum of I-c(B) is slightly shifted along the field axis, pointing to a small remanent in-plane magnetization of the F-layer along the field axis. I-c(B) of the 0-pi junction exhibits the characteristic central minimum. I-c, however, has a finite value here, due to an asymmetry of j(c) in the 0 and the pi part. In addition, this I-c(B) exhibits asymmetric maxima and bumped minima. To explain these features in detail, flux penetration being different in the 0 part and the pi part needs to be taken into account. We discuss this asymmetry in relation to the magnetic properties of the F-layer and the fabrication technique used to produce the 0-pi junctions.
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Marc 21