Broad-band 2DCS line signals equal the dc Kerr susceptibility χ(3)(Ω;Ω,0,0), which is shown to resonate at the superconductor gap frequency.
response, the broad-band pulses are modeled by delta- functions, E(t) = A1δ(t) + A2δ(t + τ ), (30) where the pulse 1 is centered at t = 0, and the pulse 2 is centered at t = −τ
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Two-dimensional coherent spectroscopy of disordered superconductors in the narrow-band and broad-band limits
Broad-band 2DCS line signals equal the dc Kerr susceptibility χ(3)(Ω;Ω,0,0), which is shown to resonate at the superconductor gap frequency.