更改

doi = 10.1142/S0218127413300024|

doi = 10.1142/S0218127413300024|

doi-access = free }}

doi-access = free }}</ref>

</ref> Self-excited attractors can be localized numerically by standard computational procedures, in which after a transient sequence, a trajectory starting from a point on an unstable manifold in a small neighborhood of an unstable equilibrium reaches an attractor, such as the classical attractors in the [[Van der Pol oscillator|Van der Pol]], [[Belousov–Zhabotinsky reaction|Belousov–Zhabotinsky]], [[Lorenz attractor|Lorenz]], and many other dynamical systems.  In contrast, the basin of attraction of a [[hidden attractor]] does not contain neighborhoods of equilibria, so the [[hidden attractor]] cannot be localized by standard computational procedures.

Self-excited attractors can be localized numerically by standard computational procedures, in which after a transient sequence, a trajectory starting from a point on an unstable manifold in a small neighborhood of an unstable equilibrium reaches an attractor, such as the classical attractors in the [[Van der Pol oscillator|Van der Pol]], [[Belousov–Zhabotinsky reaction|Belousov–Zhabotinsky]], [[Lorenz attractor|Lorenz]], and many other dynamical systems.  In contrast, the basin of attraction of a [[hidden attractor]] does not contain neighborhoods of equilibria, so the [[hidden attractor]] cannot be localized by standard computational procedures.

自激吸引子可以用标准的计算程序进行数值定域，在一个瞬态序列之后，从不稳定平衡小邻域中不稳定流形上的点开始的轨迹到达吸引子，例如[[Van der Pol振荡器| Van der Pol]]中的经典吸引子，[[Belousov–Zhabotinsky reaction | Belousov–Zhabotinsky]]，[[Lorenz吸引子| Lorenz]]，以及许多其他动力系统。相比之下，[[隐吸引子]]的吸引域不包含平衡邻域，因此[[隐吸引子]]不能用标准的计算程序进行局部化。

自激吸引子可以用标准的计算程序进行数值定域，在一个瞬态序列之后，从不稳定平衡小邻域中不稳定流形上的点开始的轨迹到达吸引子，例如[[Van der Pol振荡器| Van der Pol]]中的经典吸引子，[[Belousov–Zhabotinsky reaction | Belousov–Zhabotinsky]]，[[Lorenz吸引子| Lorenz]]，以及许多其他动力系统。相比之下，[[隐吸引子]]的吸引域不包含平衡邻域，因此[[隐吸引子]]不能用标准的计算程序进行局部化。