We study the spin-valley Kondo effect of a silicon quantum dot occupied by $% mathcal{N}$ electrons, with $mathcal{N}$ up to four. We show that the Kondo resonance appears in the $mathcal{N}=1,2,3$ Coulomb blockade regimes, but not in the $mathcal{N}=4$ one, in contrast to the spin-1/2 Kondo effect, which only occurs at $mathcal{N}=$ odd. Assuming large orbital level spacings, the energy states of the dot can be simply characterized by fourfold spin-valley degrees of freedom. The density of states (DOS) is obtained as a function of temperature and applied magnetic field using a finite-U equation-of-motion approach. The structure in the DOS can be detected in transport experiments. The Kondo resonance is split by the Zeeman splitting and valley splitting for double- and triple-electron Si dots, in a similar fashion to single-electron ones. The peak structure and splitting patterns are much richer for the spin-valley Kondo effect than for the pure spin Kondo effect.
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