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Critical temperature modification of low dimensional superconductors by spin doping”. Jalkanen P, Tuboltsev V, Virtanen A, Arutyunov K, Räisänen J, Lebedev O, Van Tendeloo G, Solid state communications 142, 407 (2007). http://doi.org/10.1016/j.ssc.2007.03.011
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Influence of strain on the tunneling magnetoresistance in diluted magnetic semiconductor trilayer and double barrier structures”. Krstajić, P, Peeters FM, Solid state communications 141, 320 (2007). http://doi.org/10.1016/j.ssc.2006.11.012
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Annular dark field imaging in a TEM”. Bals S, Kabius B, Haider M, Radmilovic V, Kisielowski C, Solid state communications 130, 675 (2004). http://doi.org/10.1016/j.ssc.2004.03.035
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Mesoscopic samples: the superconducting condensate via the Gross.Pitaevskii scenario”. Shanenko AA, Tempère J, Brosens F, Devreese JT, Solid state communications 131, 409 (2004). http://doi.org/10.1016/j.ssc.2004.03.019
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Structural transitions in a finite classical two-dimensional system”. Farias GA, Peeters FM, Solid state communications 100, 711 (1996). http://doi.org/10.1016/0038-1098(96)00438-3
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A mercury-based “1201-0201&rdquo, intergrowth HgBa2La2Cu2O8+x: a 53K superconductor”. Huvé, M, Martin C, Van Tendeloo G, Maignan A, Michel C, Hervieu M, Raveau B, Solid state communications 90, 37 (1994)
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A mercury based cuprate with the “2212&rdquo, structure: Hg2-x(Cu,Pr)xBa2PrCu2O8-\delta”. Martin C, Hervieu M, Van Tendeloo G, Goutenoire F, Michel C, Maignan A, Raveau B, Solid state communications 93, 53 (1995)
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On the superconducting phase boundary for a mesoscopic square loop”. Fomin VM, Misko VR, Devreese JT, Moshchalkov VV, Solid State Communications 101, 303 (1997)
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Stabilisation of bipolarons by polaron environment”. Shanenko AA, Smondyrev MA, Devreese JT, Solid state communications 98, 1091 (1996)
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Substitution of mercury for thallium in the 2223 cuprate: the 130K superconductor Tl1.6Hg0.4Ba2Cu3O10-x”. Goutenoire F, Maignan A, Van Tendeloo G, Martin C, Michel C, Hervieu M, Raveau B, Solid state communications 90, 47 (1994)
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