s-ordered phase-space correspondences, fermions, and negativities
APA
Dangniam, N. (2024). s-ordered phase-space correspondences, fermions, and negativities. Perimeter Institute. https://pirsa.org/24050070
MLA
Dangniam, Ninnat. s-ordered phase-space correspondences, fermions, and negativities. Perimeter Institute, May. 09, 2024, https://pirsa.org/24050070
BibTex
@misc{ pirsa_PIRSA:24050070, doi = {10.48660/24050070}, url = {https://pirsa.org/24050070}, author = {Dangniam, Ninnat}, keywords = {Quantum Foundations}, language = {en}, title = {s-ordered phase-space correspondences, fermions, and negativities}, publisher = {Perimeter Institute}, year = {2024}, month = {may}, note = {PIRSA:24050070 see, \url{https://pirsa.org}} }
For continuous-variable systems, the negativities in the s-parametrized family of quasi-probability representations on a classical phase space establish a sort of hierarchy of non-classility measures. The coherent states, by design, display no negativity for any value of -1≤s≤1, meaning that sampling from the quantum probability distribution resulting from any measurement of a coherent state can be classically simulated, placing the coherent states as the most classical states according to this particular choice of phase space.
In this talk, I will describe how to construct s-ordered quasi-probability representations for finite-dimensional quantum systems when the phase space is equipped with more general group symmetries, focusing on the fermionic SO(2n) symmetry. Along the way, I will comment on an obstruction to an analogue of Hudson's theorem, namely that the only pure states that have positive s=0 Wigner functions are Gaussian states, and a possible remedy by giving up linearity in the phase-space correspondence.
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