arXiv subjects

S. N. Coppersmith

Publications and source records attributed to S. N. Coppersmith.

119 records · Page 7Linked to original sources

arXiv2003

Dynamics of a Complex Quantum Magnet

We have computed the low energy quantum states and low frequency dynamical susceptibility of complex quantum spin systems in the limit of strong interactions, obtaining exact results for system sizes enormously larger than accessible previously. The ground state is a complex superposition of a substantial fraction of all the classical ground states, and yet the dynamical susceptibility exhibits sharp resonances reminiscent of the behavior of single spins. These results show that strongly interacting quantum systems can organize to generate coherent excitations and shed light on recent experiments demonstrating that coherent excitations are present in a disordered spin liquid. The dependence of the energy spectra on system size differs qualitatively from that of the energy spectra of random undirected bipartite graphs with similar statistics, implying that strong interactions are giving rise to these unusual spectral properties.

cond-mat.stat-mech↗

arXiv2001

Ground states of two-dimensional $\pm$J Edwards-Anderson spin glasses

We present an exact algorithm for finding all the ground states of the two-dimensional Edwards-Anderson $\pm J$ spin glass and characterize its performance. We investigate how the ground states change with increasing system size and and with increasing antiferromagnetic bond ratio $x$. We find that that some system properties have very large and strongly non-Gaussian variations between realizations.

cond-mat.stat-mech↗

arXiv2001

Weak Long-Ranged Casimir Attraction in Colloidal Crystals

We investigate the influence of geometric confinement on the free energy of an idealized model for charge-stabilized colloidal suspensions. The mean-field Poisson-Boltzmann formulation for this system predicts pure repulsion among macroionic colloidal spheres. Fluctuations in the simple ions' distribution provide a mechanism for the macroions to attract each other at large separations. Although this Casimir interaction is long-ranged, it is too weak to influence colloidal crystals' dynamics.

cond-mat.soft↗

arXiv2000

Reversible boolean networks II: Phase transition, oscillation, and local structures

We continue our consideration of a class of models describing the reversible dynamics of $N$ Boolean variables, each with $K$ inputs. We investigate in detail the behavior of the Hamming distance as well as of the distribution of orbit lengths as $N$ and $K$ are varied. We present numerical evidence for a phase transition in the behavior of the Hamming distance at a critical value $K_c\approx 1.65$ and also an analytic theory that yields the exact bounds on $1.5 \le K_c \le 2.$ We also discuss the large oscillations that we observe in the Hamming distance for $K<K_c$ as a function of time as well as in the distribution of cycle lengths as a function of cycle length for moderate $K$ both greater than and less than $K_c$. We propose that local structures, or subsets of spins whose dynamics are not fully coupled to the other spins in the system, play a crucial role in generating these oscillations. The simplest of these structures are linear chains, called linkages, and rings, called circuits. We discuss the properties of the linkages in some detail, and sketch the properties of circuits. We argue that the observed oscillation phenomena can be largely understood in terms of these local structures.

cond-mat.dis-nn↗

arXiv2000

A scalar model of inhomogeneous elastic and granular media

We investigate theoretically how the stress propagation characteristics of granular materials evolve as they are subjected to increasing pressures, comparing the results of a two-dimensional scalar lattice model to those of a molecular dynamics simulation of slightly polydisperse discs. We characterize the statistical properties of the forces using the force histogram and a two-point spatial correlation function of the forces. For the lattice model, in the granular limit the force histogram has an exponential tail at large forces, while in the elastic regime the force histogram is much narrower and has a form that depends on the realization of disorder in the model. The behavior of the force histogram in the molecular dynamics simulations as the pressure is increased is very similar to that displayed by the lattice model. In contrast, the spatial correlations evolve qualitatively differently in the lattice model and in the molecular dynamics simulations. For the lattice model, in the granular limit there are no in-plane stress-stress correlations, whereas in the molecular dynamics simulation significant in-plane correlations persist to the lowest pressures studied.

cond-mat.stat-mech↗

arXiv2000

Reversible Boolean Networks I: Distribution of Cycle Lengths

We consider a class of models describing the dynamics of $N$ Boolean variables, where the time evolution of each depends on the values of $K$ of the other variables. Previous work has considered models with dissipative dynamics. Here we consider time-reversible models, which necessarily have the property that every possible point in the state-space is an element of one and only one cycle. As in the dissipative case, when K is large, typical orbit lengths grow exponentially with N, whereas for small enough K, typical orbit lengths grow much more slowly with N. The numerical data are consistent with the existence of a phase transition at which the average orbit length grows as a power of N at a value of K between 1.4 and 1.7. However, in the reversible models the interplay between the discrete symmetry and quenched randomness can lead to enormous fluctuations of orbit lengths and other interesting features that are unique to the reversible case. The orbits can be classified by their behavior under time reversal. The orbits that transform into themselves under time reversal have properties quite different from those that do not; in particular, a significant fraction of latter-type orbits have lengths enormously longer than orbits that are time reversal-symmetric. For large K and moderate N, the vast majority of points in the state-space are on one of the time reversal singlet orbits, and a random hopping model gives an accurate description of orbit lengths. However, for any finite K, the random hopping approximation fails qualitatively when N is large enough ($N\gg 2^{(2^K)}$).

cond-mat.dis-nn↗

arXiv1998

Noise Stabilization of Self-Organized Memories

We investigate a nonlinear dynamical system which ``remembers'' preselected values of a system parameter. The deterministic version of the system can encode many parameter values during a transient period, but in the limit of long times, almost all of them are forgotten. Here we show that a certain type of stochastic noise can stabilize multiple memories, enabling many parameter values to be encoded permanently. We present analytic results that provide insight both into the memory formation and into the noise-induced memory stabilization. The relevance of our results to experiments on the charge-density wave material $NbSe_3$ is discussed.

cond-mat↗

arXiv1998

Properties of layer-by-layer vector stochastic models of force fluctuations in granular materials

We attempt to describe the stress distributions of granular packings using lattice-based layer-by-layer stochastic models that satisfy the constraints of force and torque balance and non-tensile forces at each site. The inherent asymmetry in the layer-by-layer approach appears to lead to an asymmetric force distribution, in disagreement with both experiments and general symmetry considerations. The vertical force component probability distribution is robust and in agreement with predictions of the scalar q model while the distribution of horizontal force components is qualitatively different and depends on the details of implementation.

cond-mat.soft↗

arXiv1998

Analysis of a Population Genetics Model with Mutation, Selection, and Pleiotropy

We investigate the behavior of a population genetics model introduced by Waxman and Peck incorporating mutation, selection, and pleiotropy. The population is infinite and continuous variation of genotype is allowed. Nonetheless, Waxman and Peck showed that if the degree of pleiotropy is large enough,in this model a nonzero fraction of the population can have identical alleles. This `condensed mode' behavior appears in the limit of infinite times. This paper explores the time-dependence of the distribution of alleles in this model. First, the model is analyzed using a recursion technique which enables the distribution of alleles to be calculated at finite times as well as in Waxman and Peck's infinite-time limit. Second, both Waxman and Peck's original model and a related model in which mutations occur continuously are mapped onto problems in quantum mechanics. In both cases, the long-time analysis for the biological model is equivalent to finding the nature of the eigenstates of the quantum problem. The condensed mode appears if and only if there is no bound state in the quantum problem. We compare the behavior of the discrete- and continuous-time versions of the model. The results for the two cases are qualitatively similar, though there are some quantitative differences. We also discuss our attempts to correlate the statistics of DNA sequence variations with the degree of pleiotropy of various genes.

cond-mat↗

arXiv1997

Self-Organized Short-Term Memories

We report short-term memory formation in a nonlinear dynamical system with many degrees of freedom. The system ``remembers'' a sequence of impulses for a transient period, but it coarsens and eventually ``forgets'' nearly all of them. The memory duration increases as the number of degrees of freedom in the system increases. We demonstrate the existence of these transient memories in a laboratory experiment.

cond-mat↗

arXiv1995

A Model for Force Fluctuations in Bead Packs

We study theoretically the complex network of forces that is responsible for the static structure and properties of granular materials. We present detailed calculations for a model in which the fluctuations in the force distribution arise because of variations in the contact angles and the constraints imposed by the force balance on each bead of the pile. We compare our results for force distribution function for this model, including exact results for certain contact angle probability distributions, with numerical simulations of force distributions in random sphere packings. This model reproduces many aspects of the force distribution observed both in experiment and in numerical simulations of sphere packings.

cond-mat↗