XVI CONVEGNO NAZIONALE DI FISICA STATISTICA E DEI SISTEMI COMPLESSI
con una giornata in onore di Mario Rasetti "Classical and Quantum Complexity"
Mercoledì 22 - Venerdì 24 giugno 2011, Università di Parma

programma di mercoledì 22 giugno 2011
9:30-9:50 registrazione
9:50-10:30
Alexander Blumen - Universität Freiburg (D)
Continuous time random walks and continuous time quantum walks image
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. image
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 image
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 image
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 image
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 image
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 rispostaimage
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 image
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 image
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 image
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. image
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 image
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 image
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)