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In the four-band model in Ref., the (π,π ) fluctuation favors the d x2 - y2 -wave pairing, not s± wave. The difference comes from inclusion of the d3 z2 - r2 orbital. As shown in Fig. , the presence of d3 z2 - r2 -orbital component near the Fermi level suppresses the d x2 - y2 -wave pairing due to the high density of states.
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In the four-band model in Ref., the (π, π) fluctuation favors the d x 2 - y 2 -wave pairing, not s ± wave. The difference comes from inclusion of the d 3 z 2 - r 2 orbital. As shown in Fig., the presence of d 3 z 2 - r 2 -orbital component near the Fermi level suppresses the d x 2 - y 2 -wave pairing due to the high density of states.
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Although the forth band also holds the large gap amplitude on the inner α surface, the magnitude is the same as that on the outer α surface in the third band.
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Although the forth band also holds the large gap amplitude on the inner α surface, the magnitude is the same as that on the outer α surface in the third band.
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We here define these matrix forms in different order from those in Ref., due to easier treatment of actual calculations.
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We here define these matrix forms in different order from those in Ref., due to easier treatment of actual calculations.
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