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We use a novel temperature-flow renormalization group technique to analyze magnetic and superconducting instabilities in the two-dimensional t-t^' Hubbard model for particle densities close to the Van Hove filling as a function of the next-nearest-neighbor hopping t^'. In the one-loop flow at the Van Hove filling, the characteristic temperature for the flow to strong coupling is suppressed drastically around tc^'≈-0.33t, suggesting a quantum critical point between d-wave pairing at moderate t^'>tc^' and ferromagnetism for t^'<tc^'. Upon increasing the particle density in the latter regime, the leading instability occurs in the triplet pairing channel.
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Honerkamp et al. (2001) studied this question.
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