Superconductivity at 43 K in an iron-based layered compound LaO1-xFxFeAs

By Hiroki Takahashi, Kazumi Igawa, K. Arii, Y. Kamihara, M. Hirano, Hideo Hosono. Nature, 2008

1,008 citations recorded by the source corpus.

Subfields: Accounting, Condensed Matter Physics, Electronic, Optical and Magnetic Materials

View Paper: https://www.semanticscholar.org/paper/cd01b4acea4f513dccd1d7ca0fd6949d7b910533

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In Accounting

1. G. Stewart
2. R. Greene
3. J. Paglione

In Condensed Matter Physics

1. Yang Ding
2. Lin Wang
3. Bing Li
4. H. Mao
5. Xiao-Jia Chen
6. John R. Kirtley
7. G. Stewart
8. R. Greene

In Electronic, Optical and Magnetic Materials

1. G. Stewart
2. Yang Ding
3. Lin Wang
4. Bing Li
5. Xiao-Jia Chen
6. H. Mao
7. John R. Kirtley
8. R. Greene

Citations in the corpus

• Superconductivity in iron compounds (2011, background): “Alireza et al. (2009) further reported Tc max 27 K at P ¼ 3:2 GPa for SrFe2As2, while Takahashi et al. (2008b) found Tc ð 4 GPaÞ for SrFe2As2 to be 34 K, in agreement with Igawa et al. (2009) and Kotegawa, Sugawara, and Tou (2009), the former data being displayed in Fig.”
• High-temperature superconductivity in iron-based materials (2010, background): “However three key differences are found: (1) in the arrangement of pnictogen/chalcogen anions above and below the planar iron layer (see Box 1) as opposed to the planar copper–oxygen structure of the cuprates; (2) in the ability to substitute or dope directly into the active pairing layer; and (3) i”