Nonclassical radiation in strongly driven systems originates from nonlinear dependence of the electronic dipole on the light-mode coordinate, producing squeezing or Wigner negativity depending on the order of nonlinearity.
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Tuning a femtosecond laser across the two-photon ionization threshold controls the formation of dense Rydberg gas or ultracold plasma in a Rb BEC, with charge imbalance driving the decay as confirmed by electron measurements and simulations.
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Emergence of nonclassical radiation in strongly laser-driven quantum systems
Nonclassical radiation in strongly driven systems originates from nonlinear dependence of the electronic dipole on the light-mode coordinate, producing squeezing or Wigner negativity depending on the order of nonlinearity.
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Ultrafast many-body dynamics of dense Rydberg gases and ultracold plasma
Tuning a femtosecond laser across the two-photon ionization threshold controls the formation of dense Rydberg gas or ultracold plasma in a Rb BEC, with charge imbalance driving the decay as confirmed by electron measurements and simulations.