In disordered bosonic systems, the 2D spectroscopy echo peak is controlled by the ratio of elastic to inelastic self-energies, and interaction-induced quantum fluctuations add broadening that cannot be rephased.
Squeezed Josephson plasmons in driven YBa$_2$Cu$_3$O$_{6+x}$
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abstract
The physics of driven collective modes in quantum materials underpin a number of striking non-equilibrium functional responses, which include enhanced magnetism, ferroelectricity and superconductivity. However, the coherent coupling between multiple modes at once are difficult to capture by single-pump probe (one-dimensional) spectroscopy, and often remain poorly understood. One example is phonon-mediated amplification of Josephson plasmons in YBa$_2$Cu$_3$O$_{6+x}$, in which at least three normal modes of the solid are coherently mixed as a source of enhanced superconductivity. Here, we go beyond previous pump-probe experiments in this system and acquire two-dimensional frequency maps using pairs of mutually delayed, carrier envelope phase stable mid-infrared pump pulses, combined with measurements of the time-modulated second-order nonlinear optical susceptibility. We find that the driven zone-center phonons amplify coherent pairs of opposite-momentum Josephson plasma polaritons, generating a squeezed state of interlayer phase fluctuations. The squeezed state is a potentially important ingredient in the microscopic physics of photo-induced superconductivity in this and other materials.
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Two-dimensional spectroscopy of bosonic collective excitations in disordered many-body systems
In disordered bosonic systems, the 2D spectroscopy echo peak is controlled by the ratio of elastic to inelastic self-energies, and interaction-induced quantum fluctuations add broadening that cannot be rephased.