The Relation and Evolution of Squeezing and Instability for Systems with Quadratic Hamiltonians

We propose a method that allows relating the quantum squeezing effect to the classical instability by establishing evolution equations for elements of the dispersion matrix directly in terms of elements of the stability matrix. The solution of these equations is written in terms of the evolution operator. Knowing this operator, we can analyze the system instability at finite times. Based on the developed formalism, we investigate two physical systems: the degenerate and nondegenerate parametric amplifiers with external -shaped pulses. We show that we can either amplify or, on the contrary, weaken both the squeezing effect and the system instability using -pulses.     

Fluctuations and correlations of soft gluons at the nonperturbative stage of evolution of QCD jets

At the nonperturbative stage of jet evolution, fluctuations of soft gluons are less than those for coherent states under specific conditions. This fact suggests that there can arise squeezed gluon states. The angular and rapidity dependences of the gluon correlation function are investigated at this stage of jet evolution. It is shown that these new states of soft gluons can display sub-Poissonian or super-Poissonian statistics corresponding to, respectively, antibunching and bunching of gluons, by analogy with squeezed photon states.     

Intermittency in the Ginzburg-Landau model for parton-hadron phase transitions

The formalism of squeezed states within Ginzburg-Landau theory is used to describe parton-hadron phase transitions in processes involving the production of rather high energy densities. Normalized factorial moments are studied as functions of a bin width of phase space at various squeezing parameters. The intermittency effect and scaling behavior of the moments under consideration are revealed. The values obtained for the scaling exponent agree with experimental data at small values of the squeezing parameter.