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Theory and Modern Applications

Figure 9 | Advances in Difference Equations

Figure 9

From: On the dynamics of new 4D Lorenz-type chaos systems

Figure 9

Chaotic attractors of ( 3 ) in the \(\pmb{( x_{2},w_{1},w_{2} )}\) space defined by \(\pmb{\Omega_{1,1}}\) with \(\pmb{u_{1} = 0.2}\) , \(\pmb{u_{2} = 0.5}\) , \(\pmb{q_{1} = 5.9}\) , \(\pmb{q_{2} = 9.15}\) , \(\pmb{\varepsilon_{1} = 0.5}\) , \(\pmb{\varepsilon_{2} = 0.1}\) and the initial state \(\pmb{( x_{1} ( 0 ),x_{2} ( 0 ),w_{1} ( 0 ),w_{2} ( 0 ) ) = ( 2.2,2.0,10.5,20 )}\) .

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