Abstract
On an assumption that the HO is the antiferro-quadrupolar order with Γ_{5} (Q_{z(x+y)} and Q_{z(x-y)}) symmetry, the anisotropy in temperature dependence of resistivity (ρ_{c}\propto T^{2}, and ρ_{ab}\propto T) in the HO phase of URu_2Si_2 is explained.
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