Feb 06 2018 17:11 UTC

Blake Stacey scited Post-Newtonian particle physics in curved spacetime

Jan 22 2018 21:08 UTC

Blake Stacey scited A simple explanation of Born's rule

Jan 18 2018 18:34 UTC

Blake Stacey scited Reconstruction of quantum theory from universal filters

Jan 17 2018 00:33 UTC

Blake Stacey scited Quantum Schur Sampling is Classically Tractable

Jan 17 2018 00:32 UTC

Blake Stacey scited LaVAN: Localized and Visible Adversarial Noise

Jan 16 2018 02:17 UTC

Blake Stacey scited Coherence makes quantum systems magical

Dec 17 2017 21:50 UTC

Blake Stacey scited Gravitational turbulent instability of AdS${}_5$

Dec 17 2017 21:46 UTC

Blake Stacey scited The instability of anti-de Sitter space-time

Dec 17 2017 21:43 UTC

Blake Stacey commented on Evenly distributed unitaries: on the structure of unitary designs

Neat!

Nov 23 2017 22:39 UTC

Blake Stacey scited Measurement Contextuality and Planck's Constant

Oct 17 2017 21:58 UTC

Blake Stacey scited Mysl, smysl, svet

Sep 23 2017 19:38 UTC

Blake Stacey scited Optimal simulation of state-independent quantum contextuality

Sep 20 2017 16:47 UTC

Blake Stacey scited Universally Fisher-Symmetric Informationally Complete Measurements

Aug 15 2017 16:09 UTC

Blake Stacey scited Comment on "Inferring Statistical Complexity"

Aug 02 2017 23:13 UTC

Blake Stacey scited Dimension towers of SICs. I. Aligned SICs and embedded tight frames

Jul 11 2017 16:34 UTC

Blake Stacey scited MUBs and SIC-POVMs of a spin-1 system from the Majorana approach

Jul 11 2017 16:33 UTC

Blake Stacey scited Almost quantum correlations violate the no-restriction hypothesis

Jul 11 2017 16:27 UTC

Blake Stacey commented on Fibonacci-Lucas SIC-POVMs

Eight hundred forty-four!

Jul 11 2017 16:27 UTC

Blake Stacey scited Fibonacci-Lucas SIC-POVMs

Jun 22 2017 03:02 UTC

Blake Stacey scited Reflections on the information paradigm in quantum and gravitational physics

Jun 15 2017 17:29 UTC

Blake Stacey scited Quantifying genuine multipartite correlations and their pattern complexity

Jun 15 2017 17:29 UTC

Blake Stacey scited Contextual advantage for state discrimination

Jun 14 2017 03:30 UTC

Blake Stacey scited Preprint Déjà Vu: an FAQ

Jun 08 2017 11:53 UTC

Blake Stacey scited Self-testing properties of Gisin's elegant Bell inequality

Eq. (14) defines the sum negativity as $\sum_u |W_u| - 1$, but there should be an overall factor of $1/2$ (see arXiv:1307.7171, definition 10). For both the Strange states and the Norrell states, the sum negativity should be $1/3$: The Strange states (a.k.a., Hesse SIC vectors) have one negative entry in their Wigner representation, while the Norrell states each have two negative entries of value $-1/6$. This makes the greater robustness of the Strange states under incoherent noise easy to see, because mixing in the garbage state hits the Norrell states twice as hard.