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- T K Chuan, J Maillard, K Modi, T Paterek, M Paternostro, M Piani
- Physical review letters
- 2012

The ability to distribute quantum entanglement is a prerequisite for many fundamental tests of quantum theory and numerous quantum information protocols. Two distant parties can increase the amount of entanglement between them by means of quantum communication encoded in a carrier that is sent from one party to the other. Intriguingly, entanglement can be… (More)

- N Zenine, S Boukraa, S Hassani, J.-M Maillard
- 2005

We present a simple, but efficient, way to calculate connection matrices between sets of independent local solutions, defined at two neighboring singular points, of Fuchsian differential equations of quite large orders, such as those found for the third and fourth contribution (χ and χ) to the magnetic susceptibility of square lattice Ising model. We use… (More)

- H Meyer, J.-C Angì Es D 'auriac, J.-M Maillard
- 2008

A connection between integrability properties and general statistical properties of the spectra of symmetric transfer matrices of the asymmetric eightvertex model is studied using random matrix theory (eigenvalue spacing distribution and spectral rigidity). For Yang-Baxter integrable cases, including free-fermion solutions, we have found a Poissonian… (More)

- M Bouamra, S Hassani, J.-M Maillard
- 2009

We consider some two-dimensional birational transformations. One of them is a birational deformation of the Hénon map. For some of these birational mappings, the post critical set (i.e. the iterates of the critical set) is infinite and we show that this gives straightforwardly the algebraic covariant curves of the transformation when they exist. These… (More)

We analyze free-fermion conditions on vertex models. We show –by examining examples of vertex models on square, triangular, and cubic lattices– how they amount to degeneration conditions for known symmetries of the Boltzmann weights, and propose a general scheme for such a process in two and more dimensions. SISSA–Ref. 46/96/EP PAR–LPTHE 96–08… (More)

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