Coherent states may
be of use, so they say,
but they wouldn’t be missed
if they didn’t exist.
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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).
Interpolate between thermal and coherent states.
Interpolate between thermal and coherent states.
Glauber-Sudarshan P representation of negative binomial states. K. Matsuo in Phys. Rev. A 41:519 (1990). Template:Fu97a
Interpolate between Fock and coherent states.
Gaussian states are those which can be created only with displacement operators and squeezing. See Ref. Template:Olivares12a 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]