Abstract
We argue that the hidden order (HO) state inURu2Si2 will induce a charge density wave. The modulation vector of thecharge density wave will be twice that of the hidden order state,QCDW = 2QHO.To illustrate how the charge density wave arises we use a Ginzburg–Landau theory that containsa coupling of the charge density wave amplitude to the square of the HO order parameterΔHO. This simple analysis allows us to predict the intensity and temperature dependence of thecharge density wave order parameter in terms of the susceptibilities and coupling constantsused in the Ginzburg–Landau analysis.
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