Abstract
The wave-vector integrated dynamical spin susceptibility χ 2D(ω) of YBa 2 Cu 3 O 6+y cuprates is considered. χ 2D is calculated in the superconducting state from a renormalized mean-field theory of the t−t′−J-model, based on the slave-boson formulation. Besides the well-known “41 meV resonance” a second, much broader peak ('hump') appears in Im χ 2D. It is caused by particle-hole excitations across the maximum gap Δ 0. In contrast to the resonance, which moves to lower energies when the hole filling is reduced from optimal doping, the position of this 'hump' at ≈2 Δ 0 stays almost unchanged. The results are in reasonable agreement with inelastic neutronscattering experiments.
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Brinckmann, J., Lee, P.A. Energy Scales in the Local Magnetic Excitation Spectrum of YBa2Cu3O6+y . Journal of Low Temperature Physics 126, 923–931 (2002). https://doi.org/10.1023/A:1013894608566
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DOI: https://doi.org/10.1023/A:1013894608566