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Search Results: 1 - 10 of 111858 matches for " O. Bohigas "
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Structure and Curvatures of Trajectories of a 2D Log-Gas  [PDF]
M. P. Pato, O. Bohigas
Journal of Applied Mathematics and Physics (JAMP) , 2014, DOI: 10.4236/jamp.2014.25005
Abstract: A model is constructed to study the statistical properties of irregular trajectories of a log-gas whose positions are those of the complex eigenvalues of the unitary Ginibre ensemble. It is shown that statistically the trajectories form a structure that reveals the eigenvalue departure positions. It is also shown that the curvatures of the ensemble of trajectories are Cauchy distributed.
Nuclear masses: evidence of order-chaos coexistence
O. Bohigas,P. Leboeuf
Physics , 2001, DOI: 10.1103/PhysRevLett.88.092502
Abstract: Shell corrections are important in the determination of nuclear ground-state masses and shapes. Although general arguments favor a regular single-particle dynamics, symmetry-breaking and the presence of chaotic layers cannot be excluded. The latter provide a natural framework that explains the observed differences between experimental and computed masses.
Missing levels in correlated spectra
O. Bohigas,M. P. Pato
Physics , 2004, DOI: 10.1016/j.physletb.2004.05.065
Abstract: Complete spectroscopy (measurements of a complete sequence of consecutive levels) is often considered as a prerequisite to extract fluctuation properties of spectra. It is shown how this goal can be achieved even if only a fraction of levels are observed. The case of levels behaving as eigenvalues of random matrices, of current interest in nuclear physics, is worked out in detail.
Decomposition of spectral density in individual eigenvalue contributions
O. Bohigas,M. P. Pato
Physics , 2010, DOI: 10.1088/1751-8113/43/36/365001
Abstract: The eigenvalue densities of two random matrix ensembles, the Wigner Gaussian matrices and the Wishart covariant matrices, are decomposed in the contributions of each individual eigenvalue distribution. It is shown that the fluctuations of all eigenvalues, for medium matrix sizes, are described with a good precision by nearly normal distributions.
Hyperbolic disordered ensembles of random matrices
O. Bohigas,M. P. Pato
Physics , 2011, DOI: 10.1103/PhysRev.84.031121
Abstract: Using the simple procedure, recently introduced, of dividing Gaussian matrices by a positive random variable, a family of random matrices is generated characterized by a behavior ruled by the generalized hyperbolic distribution. The spectral density evolves from the semi-circle law to a Gaussian-like behavior while concomitantly the local fluctuations show a transition from the Wigner-Dyson to the Poisson statistics. Long range statistics such as number variance exhibit large fluctuations typical of non-ergodic ensembles.
Randomly incomplete spectra and intermediate statistics
O. Bohigas,M. P. Pato
Physics , 2006, DOI: 10.1103/PhysRevE.74.036212
Abstract: By randomly removing a fraction of levels from a given spectrum a model is constructed that describes a crossover from this spectrum to a Poisson spectrum. The formalism is applied to the transitions towards Poisson from random matrix theory (RMT) spectra and picket fence spectra. It is shown that the Fredholm determinant formalism of RMT extends naturally to describe incomplete RMT spectra.
Distance matrices and isometric embeddings
E. Bogomolny,O. Bohigas,C. Schmit
Physics , 2007,
Abstract: We review the relations between distance matrices and isometric embeddings and give simple proofs that distance matrices defined on euclidean and spherical spaces have all eigenvalues except one non-negative. Several generalizations are discussed.
Quantum Chaotic Dynamics and Random Polynomials
E. Bogomolny,O. Bohigas,P. Leboeuf
Physics , 1996, DOI: 10.1007/BF02199359
Abstract: We investigate the distribution of roots of polynomials of high degree with random coefficients which, among others, appear naturally in the context of "quantum chaotic dynamics". It is shown that under quite general conditions their roots tend to concentrate near the unit circle in the complex plane. In order to further increase this tendency, we study in detail the particular case of self-inversive random polynomials and show that for them a finite portion of all roots lies exactly on the unit circle. Correlation functions of these roots are also computed analytically, and compared to the correlations of eigenvalues of random matrices. The problem of ergodicity of chaotic wave-functions is also considered. For that purpose we introduce a family of random polynomials whose roots spread uniformly over phase space. While these results are consistent with random matrix theory predictions, they provide a new and different insight into the problem of quantum ergodicity. Special attention is devoted all over the paper to the role of symmetries in the distribution of roots of random polynomials.
Spectral properties of distance matrices
E. Bogomolny,O. Bohigas,C. Schmit
Physics , 2003, DOI: 10.1088/0305-4470/36/12/341
Abstract: Distance matrices are matrices whose elements are the relative distances between points located on a certain manifold. In all cases considered here all their eigenvalues except one are non-positive. When the points are uncorrelated and randomly distributed we investigate the average density of their eigenvalues and the structure of their eigenfunctions. The spectrum exhibits delocalized and strongly localized states which possess different power-law average behaviour. The exponents depend only on the dimensionality of the manifold.
On the distribution of the total energy of a system on non-interacting fermions: random matrix and semiclassical estimates
O. Bohigas,P. Leboeuf,M. J. Sanchez
Physics , 1998,
Abstract: We consider a single particle spectrum as given by the eigenvalues of the Wigner-Dyson ensembles of random matrices, and fill consecutive single particle levels with n fermions. Assuming that the fermions are non-interacting, we show that the distribution of the total energy is Gaussian and its variance grows as n^2 log n in the large-n limit. Next to leading order corrections are computed. Some related quantities are discussed, in particular the nearest neighbor spacing autocorrelation function. Canonical and gran canonical approaches are considered and compared in detail. A semiclassical formula describing, as a function of n, a non-universal behavior of the variance of the total energy starting at a critical number of particles is also obtained. It is illustrated with the particular case of single particle energies given by the imaginary part of the zeros of the Riemann zeta function on the critical line.
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