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Ferromagnetic quantum criticality in the alloy<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="normal">Ce</mml:mi><mml:msub><mml:mi mathvariant="normal">Pd</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mo>โ</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Rh</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math>
The $\mathrm{Ce}{\mathrm{Pd}}_{1\ensuremath{-}x}{\mathrm{Rh}}_{x}$ alloy exhibits a continuous evolution from ferromagnetism $({T}_{C}=6.5\phantom{\rule{0.3em}{0ex}}\mathrm{K})$ at $x=0$ to a mixed-valence (MV) state at $x=1$. We have performed a detailed investigation on the suppression of the ferromagnetic (F) phase in this alloy using dc $({\ensuremath{\chi}}_{\mathrm{dc}})$ and ac $({\ensuremath{\chi}}_{\mathrm{ac}})$ susceptibility, specific heat $({C}_{m})$, resistivity $(\ensuremath{\rho})$, and thermal โฆ