# Communications in Nonlinear Science and Numerical Simulation

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 14-17

_{i}< 0, R

_{a}> 0). And the chaos can also appear in Burgers-Chao equations for the stable stratification (R

_{i}>...

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 32-35

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 10-14

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 48-51

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 45-48

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 43-45

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 21-27

^{α}power spectrum is robust. The lifetime distribution of electrons is found to be D(τ) = τ

^{-}

^{β}and a connection between the lifetime distribution and...

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 36-42

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 27-31

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 1 > 18-21

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 46-51

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 16-18

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 51-55

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 11-15

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 70-72

Communications in Nonlinear Science and Numerical Simulation > 1996 > 1 > 2 > 38-41

_{L}and A be the global attractor of this equation corresponding to Ω = (-L,L) and Ω = R, respectively. We show that the global attractor A is upper semicontinuity at 0 with respect to the sets {A

_{L}} in some sense.