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== Gaussian states == | == Gaussian states == | ||
Gaussian states are those which can be created only with displacement operators and squeezing. | Gaussian states are those which can be created only with displacement operators and squeezing. See Ref. {{olivares12a}} for a tutorial. | ||
Another one-mode definition is:{{cite|xu16b}} | |||
<center><wz tip="Definition of single-mode Gaussian states.">[[File:Screenshot_20250125_160250.png|400px]]</wz></center> | <center><wz tip="Definition of single-mode Gaussian states.">[[File:Screenshot_20250125_160250.png|400px]]</wz></center> | ||

This page is still in progress.
One popular characterization of quantum states is through Glauber's correlators $g^{(n)}$ (the most famous one being $g^{(2)}$). We provided a nice way to explore the Hilbert space of all quantum states using those as flashlights (see Wading through the Hilbert space).
Theoretical Aspects of Mixtures of Thermal and Coherent Radiation. G. Lachs in Phys. Rev. 138:B1012 (1965).
Gaussian states are those which can be created only with displacement operators and squeezing. See Ref. Quantum optics in the phase space. S. Olivares in Eur. Phys. J. Spec. Top. 203:3 (2012). for a tutorial.
Another one-mode definition is:[1]
A Gaussian state is pure iff the determinant of the coherence variance matrix = 1.[2][3]
Pure states having thermal photon distribution revisited: generation and phase-optimization. B. Baseia, C. M. Dantas and M. Moussa in Physica A 258:203 (1998).