| 9:30-9:50 | registrazione | 
| 9:50-10:30 | Alexander	Blumen -	Universität Freiburg (D)   
Continuous time random walks and continuous time quantum walks   
Recent years have seen a growing interest in dynamical quantum 
processes; thus it was
found that the electronic energy transfer through photosynthetic 
antennae displays quantum
features, aspects known from the dynamics of charge carriers 
along polymer backbones and
of excitations in quantum gases. Hence, in modelling energy 
transfer one has to extend the
classical, master-equation-type formalism and incorporate 
quantum-mechanical aspects, while
still taking into account the complex network of molecules over 
which the transport takes
place.
 Interestingly, the continuous time random walk (CTRW) scheme, widely employed in modelling transport in random environments, is mathematically very close to quantum- mechanical Hamiltonians of tight-binding type[1]; a simple way to see it is to focus on the time-evolution operators in statistical and in quantum mechanics: The transformation to the quantal domain leads then to continuous-time quantum walks (CTQWs). Now, while the CTQW problem is then linear, and thus many results obtained in solving CTRWs (such as eigenvalues and eigenfunctions) can be readily reutilized for CTQWs, the physically relevant properties of the two models differ vastly: In the absence of traps CTQWs are time-inversion symmetric and no energy equipartition takes place at long times. Also, the quantum system keeps memory of the initial conditions, a fact exemplified by the occurrence of quasi-revivals [1]. In this talk we will discuss this and additional features, such as the topology dependence of CTQWs, ranging from very efficient transport on regular lattices [2] to localization and trapping effects on small-world networks [3] and on fractal and hyperbranched structures [4]. We will furthermore compare the CTQW results to the corresponding CTRW results on topologically equivalent networks. This allows us to systematically explore the similarities and differences between purely classical and purely quantum-mechanical processes [1, 4]. [1] O. Mülken and A. Blumen; Phys. Rev. E 71, 036128 (2005); Phys. Rev. E 73, 066117 (2006); Physics Reports 502, 37 (2011) [2] O. Mülken, V. Bierbaum, and A. Blumen; J. Chem. Phys. 124, 124905 (2006). [3] O. Mülken, V. Pernice, and A. Blumen; Phys. Rev. E 76, 051125 (2007) [4] E. Agliari, A. Blumen, and O. Mülken; J. Phys. A 41, 445301 (2008); Phys. Rev. A 82, 012305 (2010); Intern. J. Bifurc. Chaos, 20, 271 (2010) | 
| 10:30-10:50 | Alessandro	Silva	- ICTP Trieste	 
Statistics of the work done in a quantum quench, universality and the 
critical Casimir effect.   	
I  discuss a few complementary 
characterizations of the response of a strongly correlated 
quantum system to a sudden quench of one of its control 
parameters.  After exploring various intriguing connections 
between quantum quenches, X-ray edge singularities and the 
Critical Casimir effect, I focus on quantum critical systems 
and describe in detail how universality is encoded in the 
fidelity susceptibility, in the statistics of the work done in 
a quench at low energies and in the asymptotics of correlators 
out of equilibrium.
 | 
| 10:50-11:10 | Pierpaolo Vivo - ICTP Trieste	 	
Phase transitions in the quantum 
transport problem   
	Linear statistics on ensembles of 
random matrices occur frequently in many applications. I 
present a general method to compute probability distributions 
of linear statistics for large matrix size N. This is applied 
to the calculation of full probability distribution of 
conductance and shot noise for ballistic scattering in chaotic 
cavities, in the limit of large number of open electronic 
channels. The method is based on a mapping to a Coulomb gas 
problem in Laplace space, displaying phase transitions as the 
Laplace parameter is varied. As a consequence, the sought 
distributions generally display a central Gaussian region 
flanked on both sides by non-Gaussian tails, and weak 
non-analytic points at the junction of the two regimes. I also 
briefly discuss the case of Andreev reflection between a 
normal-superconductor interface in the random 
scattering-matrix approach.
 | 
| 11:10-11:40 | pausa | 
| 11:40-12:20 | Mario	Nicodemi - Università di Napoli Federico II	
 
Symmetry Breaking at X-Chromosome Inactivation   	
In 
female mammal embryo, X-Chromosome Inactivation is the vital 
process whereby each cell inactivates one, randomly selected X 
to equalize X products w.r.t. males. Such a chromosome wide 
stochastic regulation has attracted substantial interests 
because it is unknown how the X's undergo random, yet opposite 
fates. We proposed a possible physical explanation: a Symmetry 
Breaking mechanism, with a related set of new 'particles' 
involved and a corresponding phase diagram. Our model, 
confirmed by recent experiments in Harvard, describes how a 
'blocking' complex, responsible for protecting the bound X 
from inactivation, is self-assembled and why only one is 
formed out of many diffusible molecules, resulting in a 
spontaneous symmetry breaking in the binding to two identical 
X's.
 | 
| 12:20-12:40 | Silvio	de Siena - Università di Salerno  		
Allometry and growth: a unified view	   
Allometry is crucial 
in biology - scaling relations are implied in laws of growth 
of living systems. The self similarity of Gompertzian growths 
of biological organisms plays a key role, in this regard, in 
biological similitude. The origin of allometric relationships 
and values of the scaling exponents is a source of debate; as 
well as the origin of the range of biological scales. 
Encompass these aspects in a unified view is an interesting 
target. We propose a coarse but significant model. The model 
assumes underlying fluctuations as the origin of both 
(allometry and growth) and generates the biological sizes 
through Gompertz maps. The scheme works as well for 
astrophysical structures. The inclusion of so different 
systems suggests applications to fields where allometry is 
emerging, as economy, urban planning and the social sciences. 
The deep origin and a better understanding of the stochastic 
background is the challenging goal of future investigations.
 | 
| 12:40-13:00 | Rachele	Nerattini - Università di Firenze  
On a microcanonical relation between continuous and discrete spin models   
Energy landscape methods make use of the stationary points of the energy function of a system to infer some of its collective properties. Recently this approach has been applied to equilibrium phase transitions, showing that a connection between some properties of the energy landscape and the occurrence of a phase transition exists at least for certain classes of models. We considered classical spin models and found that a relation between a class of stationary points of the energy landscape of continuous spin models on a lattice and the configurations of a Ising model defined on the same lattice exists and suggests an approximate expression for the microcanonical density of states in terms of the energy density of the Ising model. Assuming this approximation is correct close to the phase transition implies that the critical energy density of a O(n) model with ferromagnetic interactions on a lattice is equal to that of the n = 1 case, i.e., a system of Ising spins with the same interactions. This holds true in the case of long-range interactions, and at least in the special case of the mean-field XY model the expression of the density of states in terms of the Ising one can be exactly derived. For nearest-neighbor interactions, numerical results are consistent with the equality of critical energy densities for n = 2 and n = 3 in three dimensions. According to the approximation, also the critical energy of the Berezinskij-Kosterlitz-Thouless (BKT) transition for n = 2 in two dimensions (XY model) should be equal to that of the two-dimensional Ising model. However, numerical results show that the critical energies of these two models are different, although close, the difference being around 2%. The transition energies may be really equal for all cases but the BKT one, due to very different nature of the BKT phase transitions with respect to the ferromagnetic one; otherwise, transition energies might be equal only for the long-range case and different in all the other cases, with a difference that is very small and not masked by numerical errors only in the BKT case. Numerical investigations will hopefully help to clarify this point. Reference: PRL 106, 057208 (2011)
 | 
| 13:00-14:30 | pausa pranzo | 
| 14.30-15.30 | sessione poster | 
| 15:30-15:50 | Matteo	Colangeli -  Politecnico di Torino	 	
Metodi di operatori di proiezione in teoria della risposta  	
È noto che i volumi degli spazi di fase, nei 
sistemi dinamici dissipativi, contraggano (in media) e,
 
pertanto, il supporto della misura invariante risulta essere 
un attrattore frattale. Seguendo i lavori di 
vari Autori [cf. 
D. Ruelle, General linear response formula in statistical 
mechanics, and the 
fluctuation-dissipation theorem far from 
equilibrium, Physics Letters A (1998)], questo potrebbe 
indurre a 
credere che alcune serie limitazioni affliggano la 
validità dei teoremi di fluttuazione-dissipazione in 
meccanica 
statistica. In questo Lavoro, mostriamo come, in realtà, la 
Fisica riguardi essenzialmente 
la proiezione della dinamica da 
sistemi alto-dimensionali a sistemi con pochi gradi di 
libertà . Questa 
procedura di proiezione riduce grandemente la 
possibilità di incontrare situazioni "patologiche" nelle 
applicazioni.
 | 
| 15:50-16:10 | Alessio	Turchi	Università di Firenze	 	
Dynamics and equilibrium properties of β-HMF long range 
model
  	
Long range interacting systems have been found to possess unique 
equilibrium and out-of-equilibrium features, but still now 
there are only a few applications to real physical systems. 
The new  β-HMF model we propose here is a modification of 
the 
well known HMF toy-model by adding a continuous range 
parameter, thus trying to extend its applicability. This model 
has a completely different dynamic and shows interesting 
self-organization properties. At equilibrium it 
self-consistently defines a crystal lattice at low energies 
and shows multiple phase transitions between different 
thermodynamical states characterized by different structures. 
Even if the dynamics of the model are completely different 
from the HMF we were able to recover many features from that 
model. We were able to solve the model analytically for finite 
sizes and obtain the equilibrium distribution function. 
Results show that the HMF magnetization transition curve is 
perfectly reproduced for a wide range of parameters, thus 
showing thermodynamical equivalence to the HMF.
 | 
| 16:10-16:30 | Stefano	Pierini	Università di Napoli Parthenope	
 	
Coherence resonance and stochastic tipping points in climate 
dynamics
  
The concepts of relaxation oscillation and
excitable system play a fundamental role in
explaining abrupt climate changes such as the
glacial terminations and the Dansgaard-Oeschger
events on the millennial time scale, and the
Kuroshio Extension (KE) bimodal variability on a
much smaller (decadal) time scale. A crucial
aspect currently under debate is whether these
abrupt transitions are associated with a global
bifurcation (or "tipping point") being exceeded,
in which case precursors could be identified, or
if they are rather excited by fast "noise" 
dynamics through the 
coherence resonance (CR)
mechanism, with an external periodic forcing
(e.g., a Milankovitch cycle) possibly acting as a pacemaker.
 In this communication these aspects are considered in the context of the KE bimodality, chosen as a significant oceanic case study. Results of numerical simulations based on both a geophysical fluid dynamics PDE model and a low-order (4D) ODE model are used to investigate general phenomena such as: the intrinsically induced variability, Hopf, period-doubling and homoclinic bifurcations and transition to chaos, homoclinic orbits as relaxation oscillations and related stable and unstable manifolds, CR and phase selection. Finally, the new concept of stochastic tipping points is proposed with the aim of reconciling, at least formally, the bifurcation and CR views. | 
| 16:30-17:00 | pausa | 
| 17:00-17:40 | Maurizio	Serva -	Università dell'Aquila  		
Automated languages phylogeny from Levenshtein distance	  
The 
idea that the distance among pairs of languages can be 
evaluated from lexical differences seems to have its roots in 
the work of the French explorer Dumont D'Urville. He collected 
comparative words lists of various languages during his 
voyages aboard the Astrolabe from 1826 to 1829 and, in his 
work about the geographical division of the Pacific, he 
proposed a method to measure the degree of relation between 
languages.  The method used by the modern glottochronology, 
developed by Morris Swadesh in the 1950s, measures distances 
from the percentage of shared cognates, which are words with a 
common historical origin. The weak point of this method is 
that subjective judgment plays a relevant role. In fact, even 
if cognacy decisions are made by trained and experienced 
linguists, they typically vary for different authors.  
Recently, we have proposed a new automated method which is 
motivated by the analogy with genetics. The new approach has 
some advantages: the first is that it avoids subjectivity, the 
second is that results can be replicated by other scholars 
assuming that the database is the same, the third is that it 
is not requested a specific expertize in linguistic, and the 
last, but surely not the least, is that it allows for a rapid 
comparison of a very large number of languages. The distance 
between two languages is defined by considering a renormalized 
Levenshtein distance between pair of words with the same 
meaning and averaging on the words contained in a list. The 
renormalization, which takes into account the length of the 
words, plays a crucial role, and no sensible results can be 
found without it.  In this paper we give a short review of our 
automated method and we illustrate it by the Indo-European 
family and the cluster of Malagasy dialects, showing in both 
cases that it is able find out new important aspects of the 
languages relationships.
 | 
| 17:40-18:00 | Stefano	Luccioli -	CNR-ISC Firenze	 	
Discrete 
breathers as energy-accumulating centres in a protein model.	
  
We report the results of molecular dynamics simulations of an 
off-lattice protein model featuring a physical force-field and 
amino-acid sequence. We show that localised modes of nonlinear 
origin, discrete breathers (DB), emerge naturally as 
continuations of a subset of high-frequency normal modes 
residing at specific sites dictated by the native fold. In the 
case of the small beta-barrel structure that we consider, 
DB-mediated localization occurs on the turns connecting the 
strands. At high energies, discrete breathers stabilise the 
structure by concentrating  energy on few sites, while their 
collapse marks the onset of large-amplitude fluctuations  of 
the protein. Furthermore, we show how breathers develop as 
energy-accumulating centres following perturbations even at 
distant locations, thus mediating efficient and irreversible 
energy transfers. Remarkably, due to the presence of angular 
potentials, the  breather induces a local static distortion of 
the native fold. Altogether, the combination of this two 
nonlinear effects may provide a ready means for remotely 
controlling local conformational changes in proteins.  Ref: S. 
Luccioli, A. Imparato, S. Lepri, F. Piazza and A. Torcini, 
"Discrete breathers in a realistic coarse-grained model of 
proteins", to appear in Physical Biology 2011.
 | 
| 18:00-18:20 | Mario Alberto Annunziata - CNR-ISC Roma  
Segregation as a phase transition in granular matter   
We present extensive Monte Carlo simulations on species segregation in a granular mixture of hard spheres 
subjected to vertical tap. By varying the diameter ratio σ and the density ratio ρ, we find 
Brazil Nut effect (larger particles on top, BN) and Reverse Brasil Nut effect (larger particles on bottom, RBN) 
and we show that the BN - RBN passage can turn into a second-order phase transition. Further, from the 
(σ, ρ)-phase diagram of the system we find a generalisation of Archimedes’ principle for 
granular matter.
 | 
| 18:20-18:40 | Leonardo Banchi - Università di Firenze  
Ballistic quantum information transfer and effective entangling gate through homogeneous quantum wires   
Effective quantum-state and entanglement transfer can be obtained by inducing a coherent dynamics in quantum
wires with homogeneous intrawire interactions [1,2]. This goal is accomplished by optimally tuning the
coupling between the wire endpoints and the two qubits there attached. A general procedure to determine such
value is devised, and scaling laws between the optimal coupling and the length of the wire are found. The
procedure is implemented in the case of a wire consisting of a spin-1/2 XY chain: results for the time
dependence of the quantities which characterize quantum-state and entanglement transfer are found of
extremely good quality also for very long wires. The present approach neither requires engineered intrawire
interactions nor a specific initial pulse shaping, and can be applied to any quantum channels interacting
through a quasi-free Hamiltonian, i.e. an Hamiltonian that can be cast into a quadratic form in terms of some
creation and annihilation operator.  Thanks to the above optimization procedure, the transmission quality is not substantially affected by the initial state of the wire. However, in general without optimization and with more complex interacting Hamiltonians, the transmission strongly depends also on the initial state, which hence has to be engineered [3]. The proposed scheme is not only suitable for transmitting states from one wire endpoint to the other one, but it can also be used for exchanging information between the endpoints contemporaneously. In particular, in Ref. [4] we show that the optimal dynamics described in the previous section generates an effective entangling gate between the distant endpoints, and permits hence to create long-distance entanglement. References[1] L. Banchi, T. J. G. Apollaro, A. Cuccoli, R. Vaia, P. Verrucchi, Phys. Rev. A 82, 052321, (2010). [2] L. Banchi, T. J. G. Apollaro, A. Cuccoli, R. Vaia, P. Verrucchi, arXiv:1105.6058 [3] A. Bayat, L. Banchi, S. Bose, P. Verrucchi, arXiv:1104.0718 [4] L. Banchi, A. Bayat, P. Verrucchi, S. Bose, Phys. Rev. Lett. 106, 140501, (2011) |