8 research outputs found
Production and transfer of energy and information in Hamiltonian systems
We present novel results that relate energy and information transfer with sensitivity to initial conditions in chaotic multi-dimensional Hamiltonian systems. We show the relation among Kolmogorov-Sinai entropy, Lyapunov exponents, and upper bounds for the Mutual Information Rate calculated in the Hamiltonian phase space and on bi-dimensional subspaces. Our main result is that the net amount of transfer from kinetic to potential energy per unit of time is a power-law of the upper bound for the Mutual Information Rate between kinetic and potential energies, and also a power-law of the Kolmogorov-Sinai entropy. Therefore, transfer of energy is related with both transfer and production of information. However, the power-law nature of this relation means that a small increment of energy transferred leads to a relatively much larger increase of the information exchanged. Then, we propose an ?experimental? implementation of a 1-dimensional communication channel based on a Hamiltonian system, and calculate the actual rate with which information is exchanged between the first and last particle of the channel. Finally, a relation between our results and important quantities of thermodynamics is presented
Quantum criticality in ferroelectrics
Materials tuned to the neighbourhood of a zero temperature phase transition
often show the emergence of novel quantum phenomena. Much of the effort to
study these new effects, like the breakdown of the conventional Fermi-liquid
theory of metals has been focused in narrow band electronic systems.
Ferroelectric crystals provide a very different type of quantum criticality
that arises purely from the crystalline lattice. In many cases the
ferroelectric phase can be tuned to absolute zero using hydrostatic pressure or
chemical or isotopic substitution. Close to such a zero temperature phase
transition, the dielectric constant and other quantities change into radically
unconventional forms due to the quantum fluctuations of the electrical
polarization. The simplest ferroelectrics may form a text-book paradigm of
quantum criticality in the solid-state as the difficulties found in metals due
to a high density of gapless excitations on the Fermi surface are avoided. We
present low temperature high precision data demonstrating these effects in pure
single crystals of SrTiO3 and KTaO3. We outline a model for describing the
physics of ferroelectrics close to quantum criticality and highlight the
expected 1/T2 dependence of the dielectric constant measured over a wide
temperature range at low temperatures. In the neighbourhood of the quantum
critical point we report the emergence of a small frequency independent peak in
the dielectric constant at approximately 2K in SrTiO3 and 3K in KTaO3 believed
to arise from coupling to acoustic phonons. Looking ahead, we suggest that in
ferroelectric materials supporting mobile charge carriers, quantum paraelectric
fluctuations may mediate new effective electron-electron interactions giving
rise to a number of possible states such as superconductivity.Comment: 10 pages, 4 figure
Edge Stability and Transport Control with Resonant Magnetic Perturbations in Collisionless Tokamak Plasmas
A critical issue for fusion plasma research is the erosion of the first wall of the experimental device due to impulsive heating from repetitive edge magneto-hydrodynamic (MHD) instabilities known as 'edge-localized modes' (ELMs). Here, we show that the addition of small resonant magnetic field perturbations completely eliminates ELMs while maintaining a steady-state high-confinement (H-mode) plasma. These perturbations induce a chaotic behavior in the magnetic field lines, which reduces the edge pressure gradient below the ELM instability threshold. The pressure gradient reduction results from a reduction in particle content of the plasma, rather than an increase in the electron thermal transport. This is inconsistent with the predictions of stochastic electron heat transport theory. These results provide a first experimental test of stochastic transport theory in a highly rotating, hot, collisionless plasma and demonstrate a promising solution to the critical issue of controlling edge instabilities in fusion plasma devices