Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Optics Communications

New optical field and its Wigner function obtained by partial tracing over one- and two-mode combinatorial squeezed state

Wang Tong-Tong, Hong-Yi Fan

Published Jul 14, 2016• 1 citation
Publisher
DOI
10.1016/j.optcom.2016.06.054

Related papers

New Optical Field Generated by Partial Tracing Over Two-Mode Squeezing–Rotating Entangled Vacuum State $$^{{*}}$$ ∗

Gang Ren, Jian-ming Du, Wen‐Hai Zhang

Journal of Low Temperature Physics•Feb 6, 2018•2 citations

The Wigner Function and the Husimi Function of the One- and Two-Mode Combination Squeezed State

Qin Guo

International Journal of Theoretical Physics•Jun 5, 2007•5 citations

Quantum State Generated by Parity-Squeezing Combinatorial Operator and Its Wigner Function and Husimi Function

Jian-ming Du, Hai-jun Yu, Zhongquan Wang +1 more

International Journal of Theoretical Physics•Nov 19, 2010•0 citations

Wigner Distribution Function for Optical Fields and its Application to the Detection of Squeezed States

Jagdish Rai, Ramarao Inguva, Charles M. Bowden

Springer eBooks•Jan 1, 1990•0 citations

The Wigner Function of One-mode Rotated and Squeezed State

HU Xiao-guang

In this paper,we propose a new kind of one-mode rotated and squeezed state,figure out its wigner function by virtue of the presented wigner operator,and further give the corresponding wigner marginal distribution.From the distribution,we can see that the marginal distribution of this squeezed state in coordinate or momentum space is the gaussian distribution.

Acta Sinica Quantum Optica•Jan 1, 2008•0 citations

Wigner Function of a Special Type of Squeezed Coherent State

Jun Song, Hong-Yi Fan

International Journal of Theoretical Physics•Aug 1, 2011•4 citations
New Optical Field Generated by Partial Tracing Over Two-Mode Squeezing–Rotating Entangled Vacuum State ∗^{{*}}∗ ∗