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1.
Phys Rev E Stat Nonlin Soft Matter Phys ; 85(5 Pt 1): 051908, 2012 May.
Article in English | MEDLINE | ID: mdl-23004789

ABSTRACT

Transverse relaxation by dephasing in an inhomogeneous field is a general mechanism in physics, for example, in semiconductor physics, muon spectroscopy, or nuclear magnetic resonance. In magnetic resonance imaging the transverse relaxation provides information on the properties of several biological tissues. Since the dipole field is the most important part of the multipole expansion of the local inhomogeneous field, dephasing in a dipole field is highly important in relaxation theory. However, there have been no analytical solutions which describe the dephasing in a magnetic dipole field. In this work we give a complete analytical solution for the dephasing in a magnetic dipole field which is valid over the whole dynamic range.


Subject(s)
Magnetic Fields , Physical Phenomena , Magnetic Resonance Imaging
2.
Phys Rev E Stat Nonlin Soft Matter Phys ; 79(5 Pt 2): 056207, 2009 May.
Article in English | MEDLINE | ID: mdl-19518536

ABSTRACT

A network of chaotic units is investigated where the units are coupled by signals with a transmission delay. Any arbitrary finite network is considered where the chaotic trajectories of the uncoupled units are a solution of the dynamic equations of the network. It is shown that chaotic trajectories cannot be synchronized if the transmission delay is larger than the time scales of the individual units. For several models the master stability function is calculated which determines the maximal delay time for which synchronization is possible.

3.
Phys Rev E Stat Nonlin Soft Matter Phys ; 76(3 Pt 1): 031915, 2007 Sep.
Article in English | MEDLINE | ID: mdl-17930279

ABSTRACT

A method describing NMR-signal formation in inhomogeneous tissue is presented which covers all diffusion regimes. For this purpose, the frequency distribution inside the voxel is described. Generalizing the results of the well-known static dephasing regime, we derive a formalism to describe the frequency distribution that is valid over the whole dynamic range. The expressions obtained are in agreement with the results obtained from Kubos line-shape theory. To examine the diffusion effects, we utilize a strong collision approximation, which replaces the original diffusion process by a simpler stochastic dynamics. We provide a generally valid relation between the frequency distribution and the local Larmor frequency inside the voxel. To demonstrate the formalism we give analytical expressions for the frequency distribution and the free induction decay in the case of cylindrical and spherical magnetic inhomogeneities. For experimental verification, we performed measurements using a single-voxel spectroscopy method. The data obtained for the frequency distribution, as well as the magnetization decay, are in good agreement with the analytic results, although experiments were limited by magnetic field gradients caused by an imperfect shim and low signal-to-noise ratio.


Subject(s)
Magnetic Resonance Imaging , Diffusion , Fourier Analysis , Magnetics , Markov Chains , Mass Spectrometry , Models, Biological , Models, Statistical , Models, Theoretical , Normal Distribution , Phantoms, Imaging , Stochastic Processes , Time Factors
4.
Eur Phys J E Soft Matter ; 16(1): 81-7, 2005 Jan.
Article in English | MEDLINE | ID: mdl-15688144

ABSTRACT

Measurements of very slow diffusive processes in membranes, like the diffusion of integral membrane proteins, by fluorescence recovery after photo bleaching (FRAP) are hampered by bleaching of the probe during the read out of the fluorescence recovery. In the limit of long observation time (very slow diffusion as in the case of large membrane proteins), this bleaching may cause errors to the recovery function and thus provides error-prone diffusion coefficients. In this work we present a new approach to a two-dimensional closed form analytical solution of the reaction-diffusion equation, based on the addition of a dissipative term to the conventional diffusion equation. The calculation was done assuming (i) a Gaussian laser beam profile for bleaching the spot and (ii) that the fluorescence intensity profile emerging from the spot can be approximated by a two-dimensional Gaussian. The detection scheme derived from the analytical solution allows for diffusion measurements without the constraint of observation bleaching. Recovery curves of experimental FRAP data obtained under non-negligible read-out bleaching for native membranes (rabbit endoplasmic reticulum) on a planar solid support showed excellent agreement with the analytical solution and allowed the calculation of the lipid diffusion coefficient.


Subject(s)
Cell Membrane/chemistry , Cytochrome P-450 Enzyme System/chemistry , Fluorescence Recovery After Photobleaching/methods , Membrane Fluidity , Membrane Proteins/chemistry , Microsomes, Liver/chemistry , Models, Biological , Models, Chemical , Animals , Cells, Cultured , Computer Simulation , Cytochrome P-450 Enzyme System/analysis , Diffusion , Membrane Proteins/analysis , Rabbits
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