2020
DOI: 10.1103/physreva.102.063117
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Adiabatic elimination in strong-field light-matter coupling

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Cited by 16 publications
(6 citation statements)
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“…Despite the fact that this method has been used to investigate the effective dynamics in squeezed-lightenhanced atom interferometry [18], adiabatic elimination for strong field light matter coupling [19], third-order diffraction in Raman scattering [20], etc., it does not include the cavity modes. In this approach, they have worked in interaction picture and to make the Hamiltonian time independent, a suitable transformation has been utilized, which will be difficult to obtain when the cavity interactions are present.…”
Section: Iic Integro-differential Equation Approach Of Paulisch Et Almentioning
confidence: 99%
“…Despite the fact that this method has been used to investigate the effective dynamics in squeezed-lightenhanced atom interferometry [18], adiabatic elimination for strong field light matter coupling [19], third-order diffraction in Raman scattering [20], etc., it does not include the cavity modes. In this approach, they have worked in interaction picture and to make the Hamiltonian time independent, a suitable transformation has been utilized, which will be difficult to obtain when the cavity interactions are present.…”
Section: Iic Integro-differential Equation Approach Of Paulisch Et Almentioning
confidence: 99%
“…The uniform bias magnetic field excites the Kittel mode in the YIG spheres and establishes a strong photon-magnon coupling. At the large detuning regime, the common photon mode can be adiabatically eliminated with the standard perturbation theory [42][43][44] or the high-order Fermi golden rule [45]. By periodically modulating over the three magnon modes with wellcontrolled intensities, frequencies, and phases, we can obtain an effective time-reversal symmetry broken Hamiltonian [46], that ensures chiral magnon currents [38] of arbitrary states within a state-independent period.…”
Section: Introductionmentioning
confidence: 99%
“…In situations in which strongly off-resonant "virtual" states mediate interactions between quasiresonant "real" states, an adiabatic elimination over the fast degrees of freedom-the virtual ones-allows one to reduce the dimensionality of the problem and obtain an effective description of the slow degrees of freedom, i.e., the real states. This technique of adiabatic elimination, which can be formulated in several alternative ways-e.g., the Schrieffer-Wolff transformation [2]-is ubiquitous in the description and design of quantum phenomena, e.g., quantum optical applications in atomic physics [5][6][7][8][9][10][11][12][13][14][15] or exotic dynamics in the ultrastrong coupling regime of cavity QED [16][17][18]. A significant effort has been made to establish the mathematical foundations of this technique [19][20][21] and its extension to dissipative contexts for its application in open quantum systems [22][23][24][25].…”
Section: Introductionmentioning
confidence: 99%