a simple superconductor?

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Metal – Insulator Transition in Fe 1.01-x Cu x Se Cu doping changes the Fe-Fe distances 1% doping – no Meißner effect Mott transition can be induced above 4% Cu doping A J WilliamsJ. et Phys.: al. J. Condens. Phys.: Condens. Matter 21 Matter (2009) 305701 21 (2009) 305701 ICMR Summer School on Novel Superconductors 2009
Metal – Insulator Transition in Fe 1.01-x Cu x Se • Variation of magnetic susceptibility of the Fe 1.01−x Cu x Se samples with temperature • A clear increase in the local moment with x is observed, culminating in a spin-glass-type transition at Fe 0.89 Cu 0.12 Se, which then broadens out at higher dopings. This finding suggests that undoped FeSe <strong>superconductor</strong> is actually on the verge of an SDW ordering. A J Williams et al. J. Phys.: Condens. Matter 21 (2009) 305701 ICMR Summer School on Novel Superconductors 2009
Page 1 and 2: FeSe - a simple superconductor? Cla
Page 3 and 4: Rational Design Synthesis computati
Page 5 and 6: FeSe A key observation is that the
Page 7 and 8: Fe 1.01±0.2 Se Superconductivity d
Page 9 and 10: Fe 1.01 Se • No long range magnet
Page 11 and 12: Fe 1.01 Se below 100 K: dimer forma
Page 13 and 14: Tetra-Ortho transition in Fe 1.01 S
Page 15 and 16: FeSe: superconductivity under press
Page 17 and 18: Fe 1.01 Se under pressure: Transpor
Page 19 and 20: Fe 1.01 Se under pressure: Structur
Page 21 and 22: Fe 1.01 Se • Anomalous p- depende
Page 23 and 24: Tetragonal FeSe Shahab Naghavi with
Page 25 and 26: Fe 1.01 Se: evidence for quantum cr
Page 27 and 28: Fe 1.01 Se This finding suggests th
Page 29 and 30: Doping of FeSe Al, Ga, Sm occupies
Page 31: Metal - Insulator Transition in Fe
Page 35 and 36: What is different in FeSe compared
Page 37 and 38: Valence fluctuation - Superconducti
Page 39 and 40: Valence fluctuation - Superconducti
Page 41 and 42: Ni 1,5+ - Nickelates: Candidates? d
Page 43 and 44: Valence fluctuations in Europium-co
Page 45 and 46: Relation between structure and T IC

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