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arxiv: 1807.03008 · v1 · submitted 2018-07-09 · ❄️ cond-mat.supr-con · cond-mat.mtrl-sci· cond-mat.str-el

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From Ising resonant fluctuations to static uniaxial order in antiferromagnetic and weakly superconducting CeCo(In_{1-x}Hg_{x})₅ (x=0.01)

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classification ❄️ cond-mat.supr-con cond-mat.mtrl-scicond-mat.str-el
keywords fluctuationsantiferromagneticisingorderresonantsuperconductingcecocollinear
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CeCo(In$_{0.990}$Hg$_{0.010}$)$_{5}$ is a charge doped variant of the $d$-wave CoCoIn$_{5}$ superconductor with coexistent antiferromagnetic and superconducting transitions occurring at T$_{N}$= 3.4 K and T$_{c}$=1.4 K, respectively. We use neutron diffraction and spectroscopy to show that the magnetic resonant fluctuations present in the parent superconducting phase are replaced by collinear $c$-axis magnetic order with three-dimensional Ising critical fluctuations. No low energy transverse spin fluctuations are observable in this doping-induced antiferromagnetic phase and the dynamic resonant spectral weight predominately shifts to the elastic channel. Static ($\tau$ $>$ 0.2 ns) collinear Ising order is proximate to superconductivity in CeCoIn$_{5}$ and is stabilized through hole doping with Hg.

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