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i=45.5 and 21.6 meV, respectively.
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32
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80155127693
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Magnetic excitation peaks were fitted by using Gaussian plus linear background as a simple approximation here.
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Magnetic excitation peaks were fitted by using Gaussian plus linear background as a simple approximation here.
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33
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-1 are excluded from the fitting, since they are spurious peaks due to the instrumental noise.
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S. Wakimoto, K. Kodama, M. Ishikado, M. Matsuda, R. Kajimoto, M. Arai, K. Kakurai, F. Esaka, A. Iyo, H. Kito, H. Eisaki, and S. Shamoto, J. Phys. Soc. Jpn. JUPSAU 0031-9015 10.1143/JPSJ.79.074715 79, 074715 (2010).
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77954822227
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++ pairing from the viewpoint of, PRBMDO 1098-0121 10.1103/PhysRevB.81.060504
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+ + pairing from the viewpoint of S. Onari, H. Kontani, and M. Sato, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.81.060504 81, 060504 (R) (2010), although they assume a superconducting gap and thus the quasiparticle damping parameter larger than the experimental values.
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PRBMDO 1098-0121 10.1103/PhysRevB.81.214503
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S. Graser, A. F. Kemper, T. A. Maier, H.-P. Cheng, P. J. Hirschfeld, and D. J. Scalapino, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.81.214503 81, 214503 (2010).
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80155204285
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(in preparation). We set Uqtrs=0.46Uqt,Mrs regarded as the nearly critical parameter under the RPA scheme in normal states of this system.
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Y. Nagai (in preparation). We set U q t r s = 0.46 U q t, M r s regarded as the nearly critical parameter under the RPA scheme in normal states of this system.
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Nagai, Y.1
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41
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84862754725
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′′(E) within L<1/2, which we cannot discriminate from Q∼(1/21/20) experimentally because of a small Q-value difference owing to the long c-axis length than that of a axis.
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′′ (E) within L < 1 / 2, which we cannot discriminate from Q ∼ (1 / 2 1 / 2 0) experimentally because of a small Q-value difference owing to the long c-axis length than that of a axis.
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78649696125
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There is also a possibility of a pocket-like node on electron FS as is discussed recently [, PRBMDO 1098-0121 10.1103/PhysRevB.82.180502
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There is also a possibility of a pocket-like node on electron FS as is discussed recently [I. I. Mazin, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.82.180502 82, 180502 (R) (2010)].
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Mazin, I.I.1
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xy wave, since it increases the region where the sign of the order parameter is the same. The difference is whether the node is on electron or hole FS.
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x y wave, since it increases the region where the sign of the order parameter is the same. The difference is whether the node is on electron or hole FS.
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