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

日本物理学会講演概要集

Two-mode tomography of spatial Wigner function of light by using spatial light modulator

Katayose Hiroki, Keisuke Nishimura, Makoto Takeuchi, Takahiro Kuga

Published Jan 1, 2020• 0 citations
OpenAlex

Related papers

Efficient quantum tomography of two-mode Wigner functions

Ludmila Botelho, Reinaldo O. Vianna

arXiv:1912.12222•The European Physical Journal D•Feb 27, 2020•5 citations

Spatial Light Modulators: Single-Photon, Spatial-Mode Analyzers

Miles J. Padgett, Jonathan Leach, Barry Jack +4 more

Spatial Light Modulators (SLM) are pixellated display devices that can transform the phasefronts of the reflected light. Acting as programmable diffractive optical components they can transform between any two spatial modes and therefore form the basis of single-photon, spatial mode analyzers.

International Conference on Quantum Information•Jan 1, 2011•1 citation

Complete experimental characterization of the quantum state of a light mode via the Wigner function and the density matrix: application to quantum phase distributions of vacuum and squeezed-vacuum states

D. T. Smithey, M. Beck, J. Cooper +2 more

We have used the recently demonstrated method of optical homodyne tomography (OHT) to measure the Wigner quasiprobability distribution (Wigner function) and the density matrix for both a squeezed-vacuum and a vacuum state of a single spatial-temporal mode of the electromagnetic field. This method consists of measuring a set of probability distributions for many different Hilbert-space representations of the field-quadrature amplitude, using balanced homodyne detection, and then using tomography to obtain the Wigner function. Once the Wigner function is obtained, one can acquire the density matrix, including its complex phase. In the case of a pure state, this technique yields an experimentally determined complex wavefunction, as demonstrated here for the vacuum. The density matrix represents a complete quantum mechanical characterization of the state. From the measured density matrix we have obtained the Pegg–Barnett optical phase distribution, and from the Wigner function, the Wigner optical phase distribution.

Physica Scripta•Jan 1, 1993•156 citations

Center-of-Mass Tomography and Wigner Function for Multimode Photon States

Ivan V. Dudinets, Vladimir I. Man’ko

arXiv:1803.09064•International Journal of Theoretical Physics•Mar 5, 2018•7 citations

Encoding and decoding non-separable states of polarization and spatial mode of single photons

Behzad Khajavi, Xiaxi Cheng, K. Kebede +1 more

We prepare heralded single photons in a non-separable superposition of polarization and spatial modes using an in-beam polarization interferometer enabled by a spatial light modulator. We diagnose the quantum state using two techniques: quantum state tomography and imaging polarimetry. The results are in very good agreement with the expectations.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Mar 10, 2015•1 citation

A tomographic approach to Wigner's function

J. Bertrand, P. Bertrand

Foundations of Physics•Apr 1, 1987•339 citations
We have used the recently demonstrated method of optical homodyne tomography (OHT) to measure the Wigner quasiprobability distribution (Wigner function) and the density matrix for both a squeezed-vacuum and a vacuum state of a single spatial-temporal mode of the electromagnetic field. This method consists of measuring a set of probability distributions for many different Hilbert-space representations of the field-quadrature amplitude, using balanced homodyne detection, and then using tomography to obtain the Wigner function. Once the Wigner function is obtained, one can acquire the density matrix, including its complex phase. In the case of a pure state, this technique yields an experimentally determined complex wavefunction, as demonstrated here for the vacuum. The density matrix represents a complete quantum mechanical characterization of the state. From the measured density matrix we have obtained the Pegg–Barnett optical phase distribution, and from the Wigner function, the Wigner optical phase distribution.