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

Lecture notes in physics

Perspectives of the Dynamical Reduction Program

G. C. Ghirardi

Published Jan 1, 2001• 1 citation
Publisher
DOI
10.1007/3-540-44966-3_13

Related papers

The Dynamical Reduction Program

G. C. Ghirardi

Springer eBooks•Jan 1, 1992•4 citations

Macroscopic Reality and the Dynamical Reduction Program

G. C. Ghirardi

Springer eBooks•Jan 1, 1997•10 citations

John Stewart Bell and the Dynamical Reduction Program

G. C. Ghirardi

Springer eBooks•Jan 1, 2002•3 citations

Describing the macroscopic world: Closing the circle within the dynamical reduction program

G. C. Ghirardi, Renata Grassi, Fabio Benatti

Foundations of Physics•Jan 1, 1995•353 citations

Properties and events in a relativistic context: Revisiting the dynamical reduction program

G. C. Ghirardi

Foundations of Physics Letters•Aug 1, 1996•17 citations

Reconstructing the whole from its parts

Daniel Uzcátegui Contreras, Dardo Goyeneche

The quantum marginal problem consists in deciding whether a given set of marginal reductions is compatible with the existence of a global quantum state or not. In this work, we formulate the problem from the perspective of dynamical systems theory and study its advantages with respect to the standard approach. The introduced formalism allows us to analytically determine global quantum states from a wide class of self-consistent marginal reductions in any multipartite scenario. In particular, we show that any self-consistent set of multipartite marginal reductions is compatible with the existence of a global quantum state, after passing through a depolarizing channel. This result reveals that the complexity associated to the marginal problem can be drastically reduced when restricting the attention to sufficiently mixed marginals. We also formulate the marginal problem in a compressed way, in the sense that the total number of scalar constraints is smaller than the one required by the standard approach. This fact suggests an exponential speedup in runtime when considering semi-definite programming techniques to solve it, in both classical and quantum algorithms. Finally, we reconstruct $n$-qubit quantum states from all the $\binom{n}{k}$ marginal reductions to $k$ parties, generated from randomly chosen mixed states. Numerical simulations reveal that the fraction of cases where we can find a global state equals 1 when $5\leq n\leq12$ and $\lfloor(n-1)/\sqrt{2}\rfloor\leq k\leq n-1$, where $\lfloor\cdot\rfloor$ denotes the floor function.

arXiv:2209.14154•Sep 28, 2022•0 citations
The quantum marginal problem consists in deciding whether a given set of marginal reductions is compatible with the existence of a global quantum state or not. In this work, we formulate the problem from the perspective of dynamical systems theory and study its advantages with respect to the standard approach. The introduced formalism allows us to analytically determine global quantum states from a wide class of self-consistent marginal reductions in any multipartite scenario. In particular, we show that any self-consistent set of multipartite marginal reductions is compatible with the existence of a global quantum state, after passing through a depolarizing channel. This result reveals that the complexity associated to the marginal problem can be drastically reduced when restricting the attention to sufficiently mixed marginals. We also formulate the marginal problem in a compressed way, in the sense that the total number of scalar constraints is smaller than the one required by the standard approach. This fact suggests an exponential speedup in runtime when considering semi-definite programming techniques to solve it, in both classical and quantum algorithms. Finally, we reconstruct nnn-qubit quantum states from all the (nk)\binom{n}{k}(kn​) marginal reductions to kkk parties, generated from randomly chosen mixed states. Numerical simulations reveal that the fraction of cases where we can find a global state equals 1 when 5≤n≤125\leq n\leq125≤n≤12 and ⌊(n−1)/2⌋≤k≤n−1\lfloor(n-1)/\sqrt{2}\rfloor\leq k\leq n-1⌊(n−1)/2​⌋≤k≤n−1, where ⌊⋅⌋\lfloor\cdot\rfloor⌊⋅⌋ denotes the floor function.