Stéphane Attal : "Repeated
Quantum Interactions: Old and New"
We propose a review of the
so-called model of "repeated quantum interactions". We shall review the
physical motivations, the mathematical setup and main properties. We
shall also recall some old and new results: continuous-time limit,
model for a quantum heat bath, thermalization properties.
Guillaume Aubrun: "Thresholds
for
Random States"
We consider a model of random mixed
states on $C^d \otimes C^d$ obtained by the partial trace of a random
pure state on $C^d \otimes C^d \otimes C^s$ (where s corresponds to the
dimension of the environment).
Intuition tells us that when s is small, the resulting random mixed
state is likely to be entangled. On the other hand, when s is large,
the resulting state is likely to be almost maximally mixed (hence
separable). We obtain quantitative results in this direction by showing
that the threshold between generic entanglement and generic
separability occurs when s is between d^3
and d^3
log^2
d.
We obtain also more precise thresholds for some separability criteria,
such as the Positive Partial Transpose criterion and the Realignment
criterion.
(based on joint works with S. Szarek and D. Ye, and with I. Nechita).
Teodor Banica: "Complex Hadamard
Matrices - Probabilisitic Aspects"
One of the main problems in quantum
groups and subfactors, raised some time ago by Jones, is the
computation of the quantum invariants of the complex Hadamard matrices
H\in M_n(C). These invariants are a sequence of positive integers
c_1,c_2,c_3,.., which are best understood as being the moments of a
certain real probability measure \mu_H associated (in a quite
complicated way) to H. I will discuss the construction H->\mu_H, and
the few things that are known about it, from a random
matrix/probabilistic viewpoint.
Alexander Belton: "Quantum Random
Walks and Thermalisation"
The Attal-Pautrat model for repeated
interactions is a simple quantum-mechanical model of system-particle
interaction. This talk will begin by using the notions of operator
spaces and completely bounded maps to obtain a generalisation of it,
the quantum random walk. It will then be explained how such walks,
subject to suitable scaling, converge to certain quantum stochastic
processes, in a manner which is analogous to the convergence of a
classical random walk to Brownian motion.Inspired by an example of
Attal and Joye, this framework will be extended again to deal with
particles in a faithful, normal state. A new scaling, appropriate for
this setting, will be introduced and a thermalisation phenomenon is
demonstrated: for such walks, fewer quantum noises than might be
expected are required to describe the limit process. If time permits,
the extension to non-faithful states will be discussed.
François Chapon: "Quantum
Random Walks and Minors of
Hermitian Brownian Motion"
A result of Adler, Nordenstam
and van Moerbeke states that the process of eigenvalues of two
consecutive minors of Hermitian Brownian motion is a Markov process,
whereas if one considers more than two consecutive minors the Markov
property fails. We will see how to understand these results in a
noncommutative context by considering quantum random walks which are
discrete-time approximations of the eigenvalue processes of minors of
Hermitian Brownian motion (joint work with Manon Defosseux).
Benoit Collins: "Non-Commutative
Brownian Motions"
Nous étudions la classe des
processus non-commutatifs X_t dont les trajectoires sont presque
surement continues, tels que X_t et X_t^2-t sont des martingales. Dans
le cas commutatif, cette classe est réduite au mouvement
Brownien. Nous montrons que dans le cas non-commutatif, cette classe
est beaucoup plus grande, qu'elle contient beaucoup de mouvements
Browniens non-commutatifs connus (matriciel, q-Brownian Motion,
mouvement brownien libre). Par ailleurs nous développons un
calcul de Ito non-commutatif simplifie et l'utilisons pour donner une
caractérisation algébrique de ces mouvements Browniens,
et donner de nouveaux exemples et contre-exemples. Cet expose se base
sur un travail en préparation en collaboration avec Marius Junge.
Jason Crann: "Quantum Group
Channels and Non-Commutative Convolution"
The recent representation theory of
locally compact quantum groups has initiated a new connection between
harmonic analysis and quantum information. In this talk, we will
explore this connection by generating an intriguing class of quantum
channels for every locally compact quantum group. Turning to explicit
examples, we will discuss several properties of the resulting channels
including fixed points and entanglement preservation as well as provide
new counter-examples to two recently solved conjectures. As these
quantum group channels are implemented by a convolution type action of
trace class operators, we will finish with a discussion of the
associated module action along with its applications to quantum
information and amenability of quantum groups. This is joint work with
Matthias Neufang.
Mickael de la Salle: "Non-commutative
Lp spaces without the completely bounded approximation property"
Julien Deschamps: "Continuous-Time
Limit of Classical Repeated Interactions"
Yoann Dabrowski: "Random microstates
approach to free entropy"
Uwe Franz: "Quantum Probabilistic
Construction of Spectral triples on Compact Quantum Groups"
Motohisa Fukuda: "Additivity
questions in quantum communication"
In this talk, first we overview some
additivity questionswhich
arose from the study on quantum channels andsee how random matrix theory
came into this research.Secondly,
we understand how those additivity questions are violated.Some of the consequences, the
main idea of Hasitngs' proof andrelated
works by us are presented.Final
part of this talk is about open problems."
Dragi Karevski: "Quantum
Non-Equilibrium Steady States Induced by Repeated Interactions"
Claus Koestler: "Distributional
symmetries for Large Quantum
Systems"
In classical probability, de
Finetti type results infer conditional independence from
exchangeability or spreadability of an infinite sequence of random
variables. Recently we have transferred such results to an operator
algebraic framework and shown that a certain kind of noncommutative
independence emerges from the exchangeability or spreadability of an
infinite sequence of quantum subsystems. In particular we have found
new distributional symmetries, called 'braidability' and 'quantum
exchangeability'. My talk will introduce into some of these new
developments and is based in parts on joint work with Rolf Gohm and
Roland Speicher.
Camille Male: "Distribution of
traffics and their free product"
Ion Nechita: "Random Subspaces of
a Tensor Product and the Additivity Problem"`
We study singular values (or Schmidt
coefficients) of vectors in a random subspace of a tensor product. The
set of singular values of unit norm vectors in a random subspace is
shown to converge to a deterministic limit that we characterize with
the help of a norm arising in free probability. We show how these
results are related to the additivity question for the minimum output
entropy of random quantum channels.
Clément Pellegrini: "From
discrete to continous quantum trajectories and estimation"
Gilles Pisier: "Strong
Continuity
of the Reduced Free Product of States"
We give a different proof of Paul
Skoufranis's very recent resultshowing that the strong convergence (in
Camille Male's sense) of possibly non-commutative random variables
$X^{(k)}\to X$ is stable under reduced free product with a fixed
non-commutative random variable $Y$. In fact we obtain a more general
fact: assuming that the families $X^{(k)}=\{X_i^{(k)}\}$ and
$Y^{(k)}=\{Y_j^{(k)}\}$ are $*$-free as well as their
limits (in moments) $X =\{X_i \}$ and $Y =\{Y_j\}$, the strong
convergences $X^{(k)}\to X$ and $Y^{(k)}\to Y$ imply that of
$\{X^{(k)},Y^{(k)} \}$ to $\{X ,Y\}$. Phrased in more
striking language: the reduced free product is ``continuous" with
respect to strong convergence. The analogue for weak convergence (i.e.
convergence of all moments) is obvious.
René Schott: "Operator
calculus and invertible Clifford Appell systems: theory and application
to the n-particle fermion algebra"
Appell systems can be interpreted as
polynomial solutions of generalized heat equations. In probability
theory, they are also used to obtain non-central limit theorems.Their
analogues have been defined on Lie groups by P. Feinsilver et al., and
on quantum groups by U. Franz et al.Motivated by evolution equations on
Clifford algebras and illustrated with the n-particle fermion algebra,
we have developed a theory of invertible left and right Appell systems
for Clifford algebras of an arbitrary quadratic form. A direct
connection is also shown between blade factorization algorithms and the
construction of Appell systems in these algebras.(joint work with G.
Stacey STAPLES)
Yanqi Qiu: "The UMD constants for
a class of itereted $L_p(L_q)$ spaces"
Let $1 < p \neq q <
\infty$ and $(D, \mu) = (\{\pm 1\}, \frac{1}{2} \delta_{-1} +
\frac{1}{2}\delta_1)$. Define by recursion: $X_0 = \C$ and $X_{n+1} =
L_p(\mu; L_q(\mu; X_n))$. We show that there exist $c_1=c_1(p, q)>1$
and $ c_2 = c_2(p, q, s) > 1$, such that the $\text{UMD}_s$
constants of $X_n$'s satisfy $c_1^n \leq C_s(X_n) \leq c_2^n$ for all
$1 < s < \infty$. Our results yield an elementary construction of
super-reflexive non-$\text{UMD}$ Banach lattices.
Karol Życzkowski: "Probabilistic
approach to quantum states: Numerical Shadow of an operator"
For a matrix A of a order N one defines its
numerical shadow as a probability distribution supported on its
numerical range
W(A), induced by the unitarily
invariant Fubini--Study measure on the complex projective manifold of
pure
quantum states of size N. The notions of
numerical range and numerical shadow
can be extended for operators acting on a Hilbert space with a tensor
product
structure. Restricting the set of pure states to the set of product
states or
maximally entangled states we introduce restricted numerical range and
restricted
numerical shadow of an operator. Analyzing restricted shadows of
operators of a
fixed size N=KM we analyze the geometry of sets of separable and
maximally
entangled states of the K times M
composite quantum system.