Quantum States: Difference between revisions
Fabrice P. Laussy's Web
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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.


The precise one-mode definition is:{{cite|xu16b}}
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>



Revision as of 00:02, 27 January 2025

This page is still in progress.

Quantum States

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).

Fock states

Coherent states

Thermal states

Cothermal states

Theoretical Aspects of Mixtures of Thermal and Coherent Radiation. G. Lachs in Phys. Rev. 138:B1012 (1965).

Gaussian states

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]

Squeezing

Beyond the diagonal

Randomly phased coherent states

Pure thermal distribution

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).

References