P. N. Valdivia

Phase diagram of the PrFeAsO1 xFx superconductor

The electronic phase diagram of

Phase diagram of thePrFeAsO1−xFxsuperconductor

{\text{PrFeAsO}}_{1\ensuremath{-}x}{\text{F}}_{x}

Universal magnetic and structural behaviors in the iron arsenides

(0\ensuremath{\le}x\ensuremath{\le}0.225)

Experimental elucidation of the origin of the ‘double spin resonances’ in Ba(Fe1−xCox)2As2

has been determined using synchrotron x-ray powder-diffraction, magnetization, and resistivity measurements. The structural transition temperature is suppressed from 154 to

Magnetic order tuned by Cu substitution in Fe1.1–zCuzTe

\ensuremath{\approx}120\text{ }\text{K}

Two spatially separated phases in semiconducting Rb0.8Fe1.5S2

and the magnetic phase transitions of both iron and praseodymium ions are completely suppressed by

Spin dynamics near a putative antiferromagnetic quantum critical point in Cu-substituted BaFe2As2 and its relation to high-temperature superconductivity

x\ensuremath{\approx}0.08

The effects of post-growth annealing on the structural and magnetic properties of BaFe2As2

fluorine doping, coinciding with the emergence of superconductivity. The optimal doping is

Spin Waves and Spatially Anisotropic Exchange Interactions in the S = 2 Stripe Antiferromagnet Rb0.8Fe1.5S2

x\ensuremath{\approx}0.15