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In the (formula presented) calculation, the hybridization with the almost full-filled up-spin Cr (formula presented) orbitals induces a finite positive Mo spin, which partly counteracts the large negative Mo spin caused by the down-spin Mo (formula presented) orbitals. The Mo (formula presented) electrons are less itinerant in (formula presented) than in SFMO, which is also indicated by comparison of the down-spin Mo (formula presented) bandwidths as seen in Fig. 33
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In the (formula presented) calculation, the hybridization with the almost full-filled up-spin Cr (formula presented) orbitals induces a finite positive Mo spin, which partly counteracts the large negative Mo spin caused by the down-spin Mo (formula presented) orbitals. The Mo (formula presented) electrons are less itinerant in (formula presented) than in SFMO, which is also indicated by comparison of the down-spin Mo (formula presented) bandwidths as seen in Fig. 33.
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