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We find that Nσ (ε) = mV kσ (ε) (2 π2) -1 1-σm λ2 / h2 + λ2 kσ2 (ε), kσ (ε) = [2 (ε+μ) m+2 λ2 m2 +2σ λ4 m4 +2 λ2 m3 (ε+μ) + h2 m2] 1/2.
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We find that Nσ (ε) = mV kσ (ε) (2 π2) -1 1-σm λ2 / h2 + λ2 kσ2 (ε), kσ (ε) = [2 (ε+μ) m+2 λ2 m2 +2σ λ4 m4 +2 λ2 m3 (ε+μ) + h2 m2] 1/2.
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The nontrivial phase factor t (k) =-t (k) is defined such that T |k〉 =t (k) | -k〉, where T is the time-reversal operator.
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The nontrivial phase factor t (k) =-t (k) is defined such that T |k〉 =t (k) | -k〉, where T is the time-reversal operator.
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Experimentally, the measurements on a single crystal of UIr so far indicate that the orbital effects of the magnetic field dominate.
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Experimentally, the measurements on a single crystal of UIr so far indicate that the orbital effects of the magnetic field dominate.
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