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We report low-temperature thermal-expansion measurements on single crystals of the {\it layered} heavy fermion system \cri () and compare it with a previous study on the related {\it cubic} system \ci [R. K"{u}chler {\it et al.}, Phys. Rev. Lett. {\bf 96}, 256403 (2006)]. Both systems display a quantum critical point as proven by a divergent Gr"uneisen ratio. Most remarkably, the three-dimensional itinerant model explains quantum criticality in {\it both} systems, suggesting that the crystalline anisotropy in \cri is unimportant. This is ascribed to the effect of weak disorder in these doped systems.

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