
Using the unrestricted Hartree-Fock approximation and Landau theory we identify possible phases competing with superconductivity in FeAs layers. We find that close to half-filling the transition from the paramagnet to the magnetically ordered phase is first-order making anharmonicities relevant and leading to a rich phase diagram. Between the already known one dimensionally modulated magnetic stripe phase and the paramagnet we find a new phase which has the same structure factor as the former but in which magnetic moments at nearest-neighbor sites are at right angles making electrons to acquire a non trivial phase when circulating a plaquette at strong coupling. Another competing phase has magnetic and charge order and may be stabilized by charged impurities.
5 pages, 2 figures
MODEL, Superconductivity (cond-mat.supr-con), Physics and Astronomy (all), Condensed Matter - Strongly Correlated Electrons, Strongly Correlated Electrons (cond-mat.str-el), SUPERCONDUCTIVITY, Condensed Matter - Superconductivity, FOS: Physical sciences, SYSTEM
MODEL, Superconductivity (cond-mat.supr-con), Physics and Astronomy (all), Condensed Matter - Strongly Correlated Electrons, Strongly Correlated Electrons (cond-mat.str-el), SUPERCONDUCTIVITY, Condensed Matter - Superconductivity, FOS: Physical sciences, SYSTEM
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