scholarly journals Exact form of the exponential correlation function in the glassy super-rough phase

2013 ◽  
Vol 87 (21) ◽  
Author(s):  
Pierre Le Doussal ◽  
Zoran Ristivojevic ◽  
Kay Jörg Wiese
Geophysics ◽  
1980 ◽  
Vol 45 (9) ◽  
pp. 1351-1372 ◽  
Author(s):  
Robert Godfrey ◽  
Francis Muir ◽  
Fabio Rocca

Acoustic impedance is modeled as a special type of Markov chain, one which is constrained to have a purely exponential correlation function. The stochastic model is parsimoniously described by M parameters, where M is the number of states or rocks composing an impedance well log. The probability mass function of the states provides M-1 parameters, and the “blockiness” of the log determines the remaining degree of freedom. Synthetic impedance and reflectivity logs constructed using the Markov model mimic the blockiness of the original logs. Both synthetic impedance and reflectivity are shown to be Bussgang, i.e., if the sequence is input into an instantaneous nonlinear device, then the correlation of input and output is proportional to the autocorrelation of the input. The final part of the paper uses the stochastic model in formulating an algorithm that transforms a deconvolved seismogram into acoustic impedance. The resulting function is blocky and free of random walks or sags. Low‐frequency information, as provided by moveout velocities, can be easily incorporated into the algorithm.


2014 ◽  
Vol 2014 ◽  
pp. 1-6 ◽  
Author(s):  
Héctor Calisto ◽  
Kristopher J. Chandía ◽  
Mauro Bologna

We consider a generalized Malthus-Verhulst model with a fluctuating carrying capacity and we study its effects on population growth. The carrying capacity fluctuations are described by a Poissonian process with an exponential correlation function. We will find an analytical expression for the average of a number of individuals and show that even in presence of a fluctuating carrying capacity the average tends asymptotically to a constant quantity.


1997 ◽  
Vol 11 (01n02) ◽  
pp. 103-107
Author(s):  
A. H. Bougourzi ◽  
M. Couture ◽  
M. Kacir

The exact form factors of the Heisenberg models XXX and XXZ have been recently computed through the quantum affine symmetry of XXZ model in the thermodynamic limit. We use them to derive an exact formula for the contribution of two spinons to the dynamical correlation function of XXX model at zero temperature.


1985 ◽  
Vol 85 ◽  
pp. 249-253
Author(s):  
R. Schiffer ◽  
K.O. Thielheim

AbstractWe calculated the scattering cross section of an ensemble of large, convex, randomly oriented particles with a slight surface roughness. If the roughness structure is described by an exponential correlation function, the degree and angular dependence of the zodiacal light reddening are well reproduced by our model.


2021 ◽  
Vol 77 (1) ◽  
pp. 75-80
Author(s):  
Salvino Ciccariello

An algebraic approximation, of order K, of a polyhedron correlation function (CF) can be obtained from γ′′(r), its chord-length distribution (CLD), considering first, within the subinterval [D i−1, D i ] of the full range of distances, a polynomial in the two variables (r − D i−1)1/2 and (D i − r)1/2 such that its expansions around r = D i−1 and r = D i simultaneously coincide with the left and right expansions of γ′′(r) around D i−1 and D i up to the terms O(r − D i−1) K/2 and O(D i − r) K/2, respectively. Then, for each i, one integrates twice the polynomial and determines the integration constants matching the resulting integrals at the common end-points. The 3D Fourier transform of the resulting algebraic CF approximation correctly reproduces, at large q's, the asymptotic behaviour of the exact form factor up to the term O[q −(K/2+4)]. For illustration, the procedure is applied to the cube, the tetrahedron and the octahedron.


1992 ◽  
Vol 290 ◽  
Author(s):  
B. J. Frisken ◽  
Fabio Ferri ◽  
David S. Cannell

AbstractThe effect of even dilute silica networks on the critical phenomena of binary liquid mixtures is profound. The network preferentially adsorbs one component, preventing a portion of the mixture from participating in critical fluctuations. Fluctuations in the remaining mixture are found to decay with a non-exponential correlation function near the consolute point. A correlation function consisting of the sum of an exponential decay and a non-exponential term of either an activated or stretched exponential form fits the data well. In the presence of the silica network, the mixtures are observed to phase separate near the critical temperature of the pure system, but while still in the one-phase region of the pure system.


Author(s):  
V P Gerasimov ◽  
V D Kovalev ◽  
A Yu Darzhaniya ◽  
R A Magomedov ◽  
E V Sokolova ◽  
...  

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